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STEP3 2019 -- Pure Mathematics

Exam: STEP3  |  Year: 2019  |  Questions: Q1—Q8  |  Total marks per question: 20

All questions are pure mathematics. Solutions and examiner commentary are included below.

QTopicDifficultyKey Techniques
1纯数Challenging矩阵特征值法,消元法解ODE,相平面分析,极值点定位
2纯数Challenging极限定义推导,函数方程微分法,分离变量,双曲函数恒等式
3纯数Challenging线性代数,不变子空间理论,分类讨论,方程组求解
4纯数HardVieta公式,平方和非负性分析,整数约束下的穷举,反证法
5纯数Hard代换积分法,部分分式分解,反三角函数,积分限变换
6纯数Challenging复数模运算,反演变换几何性质,圆的方程分析,分类讨论
7纯数Challenging隐式方程分析,判别式法,导数求切线方向,曲线对称性
8纯数Challenging法向量计算,向量叉积,三角恒等式推导,不等式证明

Topic: 纯数  |  Difficulty: Challenging  |  Marks: 20

1 The coordinates of a particle at time tt are xx and yy. For t⩾0t \geqslant 0, they satisfy the pair of coupled differential equations

x˙=−x−ky\dot{x} = -x - ky y˙=x−y\dot{y} = x - y

where kk is a constant. When t=0t = 0, x=1x = 1 and y=0y = 0.

(i) Let k=1k = 1. Find xx and yy in terms of tt and sketch yy as a function of tt.

Sketch the path of the particle in the xx-yy plane, giving the coordinates of the point at which yy is greatest and the coordinates of the point at which xx is least.

(ii) Instead, let k=0k = 0. Find xx and yy in terms of tt and sketch the path of the particle in the xx-yy plane.

Hint

(i) x˙=−x−y\dot{x} = -x - y

So y=−x˙−xy = -\dot{x} - x

As y˙=x−y\dot{y} = x - y, −x¨−x˙=x+x˙+x-\ddot{x} - \dot{x} = x + \dot{x} + x

x¨+2x˙+2x=0\ddot{x} + 2\dot{x} + 2x = 0

[M1]

AQE λ2+2λ+2=0\lambda^2 + 2\lambda + 2 = 0, λ=−1±i\lambda = -1 \pm i so x=e−t(Acos⁡t+Bsin⁡t)x = e^{-t}(A \cos t + B \sin t) [M1 A1 cao]

[Alternatively, x=y˙+yx = \dot{y} + y leading to y¨+2y˙+2y=0\ddot{y} + 2\dot{y} + 2y = 0 and y=e−t(Ccos⁡t+Dsin⁡t)y = e^{-t}(C \cos t + D \sin t) etc]

So y=e−t(Acos⁡t+Bsin⁡t)−e−t(−Asin⁡t+Bcos⁡t)−e−t(Acos⁡t+Bsin⁡t)y = e^{-t}(A \cos t + B \sin t) - e^{-t}(-A \sin t + B \cos t) - e^{-t}(A \cos t + B \sin t)

=e−t(Asin⁡t−Bcos⁡t)= e^{-t}(A \sin t - B \cos t)

t=0,x=1⇒A=1t = 0, x = 1 \Rightarrow A = 1 and t=0,y=0⇒B=0t = 0, y = 0 \Rightarrow B = 0

So x=e−tcos⁡tx = e^{-t} \cos t and y=e−tsin⁡ty = e^{-t} \sin t [M1 A1 cao]

ttyy
0000
π\pi00
2π2\pi00

G1 G1 [7]

yy is greatest when y˙=0⇒x=y⇒tan⁡t=1⇒t=π4+nπ\dot{y} = 0 \Rightarrow x = y \Rightarrow \tan t = 1 \Rightarrow t = \frac{\pi}{4} + n\pi

Hence t=π4t = \frac{\pi}{4} thus (e−π42,e−π42)\left( \frac{e^{-\frac{\pi}{4}}}{\sqrt{2}}, \frac{e^{-\frac{\pi}{4}}}{\sqrt{2}} \right) [M1]

xx is least when x˙=0⇒x=−y⇒tan⁡t=−1⇒t=3π4+nπ\dot{x} = 0 \Rightarrow x = -y \Rightarrow \tan t = -1 \Rightarrow t = \frac{3\pi}{4} + n\pi

Hence t=3π4t = \frac{3\pi}{4} thus (−e−3π42,e−3π42)\left( -\frac{e^{-\frac{3\pi}{4}}}{\sqrt{2}}, \frac{e^{-\frac{3\pi}{4}}}{\sqrt{2}} \right) [M1]

G1 G1 G1 [5]

(ii) x˙=−x  ⟹  x=Ae−t\dot{x} = -x \implies x = Ae^{-t}

t=0,x=1  ⟹  A=1  ⟹  x=e−tt = 0, x = 1 \implies A = 1 \implies x = e^{-t} M1

So y˙+y=e−t\dot{y} + y = e^{-t}

The integrating factor is ete^t. Thus ety=∫1dt=t+ce^t y = \int 1 dt = t + c

y=(t+c)e−ty = (t + c)e^{-t} M1

t=0,y=0  ⟹  c=0t = 0, y = 0 \implies c = 0 so y=te−ty = te^{-t} A1 cao

dydx=y˙x˙=(1−t)e−t−e−t=t−1\frac{dy}{dx} = \frac{\dot{y}}{\dot{x}} = \frac{(1-t)e^{-t}}{-e^{-t}} = t - 1 so there is a maximum at (e−1,e−1)(e^{-1}, e^{-1}) M1

As t→∞t \to \infty, dydx→∞\frac{dy}{dx} \to \infty M1

Alternatively,

As y˙=x−y\dot{y} = x - y, y¨=x˙−y˙=−x−y˙\ddot{y} = \dot{x} - \dot{y} = -x - \dot{y}

So y¨+2y˙+y=0\ddot{y} + 2\dot{y} + y = 0 yielding y=(At+B)e−ty = (At + B)e^{-t} M1

xxyy
0000
e−1e^{-1}e−1e^{-1}
1100

G1 G1 G1 [8]

Model Solution

Part (i) (k=1k = 1)

With k=1k = 1, the system becomes x˙=−x−y\dot{x} = -x - y and y˙=x−y\dot{y} = x - y.

From the first equation, y=−x˙−xy = -\dot{x} - x, so y˙=−x¨−x˙\dot{y} = -\ddot{x} - \dot{x}.

Substituting into the second equation:

−x¨−x˙=x−(−x˙−x)=2x+x˙-\ddot{x} - \dot{x} = x - (-\dot{x} - x) = 2x + \dot{x}

x¨+2x˙+2x=0\ddot{x} + 2\dot{x} + 2x = 0

The auxiliary equation is λ2+2λ+2=0\lambda^2 + 2\lambda + 2 = 0, giving λ=−2±4−82=−1±i\lambda = \dfrac{-2 \pm \sqrt{4-8}}{2} = -1 \pm i.

So x=e−t(Acos⁡t+Bsin⁡t)x = e^{-t}(A\cos t + B\sin t).

To find yy: since y=−x˙−xy = -\dot{x} - x, we compute x˙\dot{x}:

x˙=−e−t(Acos⁡t+Bsin⁡t)+e−t(−Asin⁡t+Bcos⁡t)\dot{x} = -e^{-t}(A\cos t + B\sin t) + e^{-t}(-A\sin t + B\cos t)

=e−t[(−A+B)cos⁡t+(−A−B)sin⁡t]= e^{-t}[(-A+B)\cos t + (-A-B)\sin t]

Therefore:

y=−x˙−x=−e−t[(−A+B)cos⁡t+(−A−B)sin⁡t]−e−t(Acos⁡t+Bsin⁡t)y = -\dot{x} - x = -e^{-t}[(-A+B)\cos t + (-A-B)\sin t] - e^{-t}(A\cos t + B\sin t)

=e−t[(A−B)cos⁡t+(A+B)sin⁡t−Acos⁡t−Bsin⁡t]= e^{-t}[(A - B)\cos t + (A + B)\sin t - A\cos t - B\sin t]

=e−t(−Bcos⁡t+Asin⁡t)= e^{-t}(-B\cos t + A\sin t)

Applying initial conditions: x(0)=1x(0) = 1 gives A=1A = 1, and y(0)=0y(0) = 0 gives −B=0-B = 0, so B=0B = 0.

x=e−tcos⁡t,y=e−tsin⁡t\boxed{x = e^{-t}\cos t, \qquad y = e^{-t}\sin t}

Sketch of yy as a function of tt:

y(0)=0y(0) = 0, and y=0y = 0 whenever sin⁡t=0\sin t = 0, i.e. at t=0,π,2π,…t = 0, \pi, 2\pi, \ldots The envelope ±e−t\pm e^{-t} decays exponentially. yy reaches its first positive maximum at t=π4t = \frac{\pi}{4}, its first negative minimum at t=5π4t = \frac{5\pi}{4}, and the oscillations die away as t→∞t \to \infty.

Path in the xx-yy plane:

Note that x2+y2=e−2t(cos⁡2t+sin⁡2t)=e−2tx^2 + y^2 = e^{-2t}(\cos^2 t + \sin^2 t) = e^{-2t}, so the distance from the origin is r=e−tr = e^{-t}, which decreases monotonically. The particle spirals inward toward the origin.

Maximum yy: We need y˙=0\dot{y} = 0, i.e. x−y=0x - y = 0, so x=yx = y:

e−tcos⁡t=e−tsin⁡t  ⟹  tan⁡t=1  ⟹  t=π4+nπe^{-t}\cos t = e^{-t}\sin t \implies \tan t = 1 \implies t = \frac{\pi}{4} + n\pi

For the first (and largest) positive yy, t=π4t = \frac{\pi}{4}:

(e−π/42,  e−π/42)\left(\frac{e^{-\pi/4}}{\sqrt{2}},\; \frac{e^{-\pi/4}}{\sqrt{2}}\right)

Minimum xx: We need x˙=0\dot{x} = 0, i.e. −x−y=0-x - y = 0, so x=−yx = -y:

e−tcos⁡t=−e−tsin⁡t  ⟹  tan⁡t=−1  ⟹  t=3π4+nπe^{-t}\cos t = -e^{-t}\sin t \implies \tan t = -1 \implies t = \frac{3\pi}{4} + n\pi

For the first such value, t=3π4t = \frac{3\pi}{4}:

(−e−3π/42,  e−3π/42)\left(-\frac{e^{-3\pi/4}}{\sqrt{2}},\; \frac{e^{-3\pi/4}}{\sqrt{2}}\right)


Part (ii) (k=0k = 0)

With k=0k = 0, x˙=−x\dot{x} = -x and y˙=x−y\dot{y} = x - y.

From the first equation: x˙=−x\dot{x} = -x gives x=Ae−tx = Ae^{-t}. With x(0)=1x(0) = 1: A=1A = 1, so x=e−tx = e^{-t}.

Substituting into the second equation: y˙+y=e−t\dot{y} + y = e^{-t}.

The integrating factor is ete^t:

ddt(ety)=et⋅e−t=1\frac{d}{dt}(e^t y) = e^t \cdot e^{-t} = 1

ety=t+ce^t y = t + c

With y(0)=0y(0) = 0: c=0c = 0, so:

x=e−t,y=te−t\boxed{x = e^{-t}, \qquad y = te^{-t}}

Path in the xx-yy plane:

The path starts at (1,0)(1, 0) when t=0t = 0. As tt increases, x=e−tx = e^{-t} decreases monotonically while y=te−ty = te^{-t} increases from 0 to a maximum and then decreases back to 0.

To find the maximum yy on the curve, we compute dydx=y˙x˙=(1−t)e−t−e−t=t−1\dfrac{dy}{dx} = \dfrac{\dot{y}}{\dot{x}} = \dfrac{(1-t)e^{-t}}{-e^{-t}} = t - 1.

Setting dydx=0\dfrac{dy}{dx} = 0: t=1t = 1, giving the point (e−1,e−1)(e^{-1}, e^{-1}).

As t→∞t \to \infty, dydx=t−1→∞\dfrac{dy}{dx} = t - 1 \to \infty, meaning the tangent becomes vertical (approaching the origin along the positive xx-axis from above).

The path starts at (1,0)(1,0), rises to (e−1,e−1)(e^{-1}, e^{-1}), then curves back toward the origin.

Examiner Notes

k=0时方程退化为可分离变量形式,需注意;画轨迹图时需准确标注y最大值和x最小值的坐标。耦合ODE是STEP3高频考点。


Topic: 纯数  |  Difficulty: Challenging  |  Marks: 20

2 The definition of the derivative f′f' of a (differentiable) function ff is

f′(x)=lim⁡h→0f(x+h)−f(x)h.(*)f'(x) = \lim_{h \to 0} \frac{f(x + h) - f(x)}{h} . \qquad \text{(*)}

(i) The function ff has derivative f′f' and satisfies

f(x+y)=f(x)f(y)f(x + y) = f(x)f(y)

for all xx and yy, and f′(0)=kf'(0) = k where k≠0k \neq 0. Show that f(0)=1f(0) = 1.

Using (∗*), show that f′(x)=kf(x)f'(x) = kf(x) and find f(x)f(x) in terms of xx and kk.

(ii) The function gg has derivative g′g' and satisfies

g(x+y)=g(x)+g(y)1+g(x)g(y)g(x + y) = \frac{g(x) + g(y)}{1 + g(x)g(y)}

for all xx and yy, ∣g(x)∣<1|g(x)| < 1 for all xx, and g′(0)=kg'(0) = k where k≠0k \neq 0.

Find g′(x)g'(x) in terms of g(x)g(x) and kk, and hence find g(x)g(x) in terms of xx and kk.

Hint

(i) Let y=0y = 0, f(x+0)=f(x)f(0)∀xf(x + 0) = f(x)f(0) \forall x, so f(x)=f(x)f(0)∀xf(x) = f(x)f(0) \forall x M1

Thus f(x)(1−f(0))=0∀xf(x)(1 - f(0)) = 0 \forall x. Therefore, f(x)=0∀xf(x) = 0 \forall x, or f(0)=1f(0) = 1 M1

If f(x)=0∀xf(x) = 0 \forall x then f′(x)=0∀xf'(x) = 0 \forall x but f′(0)=k≠0f'(0) = k \neq 0 so f(0)=1f(0) = 1 A1* cso

f′(x)=lim⁡h→0(f(x+h)−f(x)h)=lim⁡h→0(f(x)f(h)−f(x)h)=f(x)lim⁡h→0(f(h)−1h)f'(x) = \lim_{h \to 0} \left( \frac{f(x+h) - f(x)}{h} \right) = \lim_{h \to 0} \left( \frac{f(x)f(h) - f(x)}{h} \right) = f(x) \lim_{h \to 0} \left( \frac{f(h) - 1}{h} \right) M1

But lim⁡h→0(f(h)−1h)=lim⁡h→0(f(0+h)−f(0)h)=f′(0)=k\lim_{h \to 0} \left( \frac{f(h) - 1}{h} \right) = \lim_{h \to 0} \left( \frac{f(0+h) - f(0)}{h} \right) = f'(0) = k so f′(x)=kf(x)f'(x) = kf(x) M1 A1* cso

Thus

f′(x)f(x)=k\frac{f'(x)}{f(x)} = k

Integrating

ln⁡(f(x))=kx+c\ln(f(x)) = kx + c

M1

So f(x)=ekx+c=Aekxf(x) = e^{kx+c} = Ae^{kx}. As f(0)=1f(0) = 1, A=1A = 1, so f(x)=ekxf(x) = e^{kx} M1 A1 cao [9]

(ii) Let y=0y = 0,

g(x+0)=g(x)+g(0)1+g(x)g(0)∀xg(x + 0) = \frac{g(x) + g(0)}{1 + g(x)g(0)} \forall x

M1

Thus g(x)+(g(x))2g(0)=g(x)+g(0)∀xg(x) + (g(x))^2 g(0) = g(x) + g(0) \forall x

So ((g(x))2−1)g(0)=0∀x((g(x))^2 - 1) g(0) = 0 \forall x M1

As ∣g(x)∣<1|g(x)| < 1, (g(x))2−1≠0(g(x))^2 - 1 \neq 0, and thus g(0)=0g(0) = 0 A1

g′(x)=lim⁡h→0(g(x+h)−g(x)h)g'(x) = \lim_{h \to 0} \left( \frac{g(x + h) - g(x)}{h} \right)

=lim⁡h→0(g(x)+g(h)1+g(x)g(h)−g(x)h)=lim⁡h→0(g(x)+g(h)−g(x)(1+g(x)g(h))h(1+g(x)g(h)))= \lim_{h \to 0} \left( \frac{\frac{g(x) + g(h)}{1 + g(x)g(h)} - g(x)}{h} \right) = \lim_{h \to 0} \left( \frac{g(x) + g(h) - g(x)(1 + g(x)g(h))}{h(1 + g(x)g(h))} \right)

M1

=lim⁡h→0(g(h)(1−(g(x))2)h(1+g(x)g(h)))=(1−(g(x))2)lim⁡h→0(g(h)h(1+g(x)g(h)))= \lim_{h \to 0} \left( \frac{g(h) (1 - (g(x))^2)}{h(1 + g(x)g(h))} \right) = (1 - (g(x))^2) \lim_{h \to 0} \left( \frac{g(h)}{h(1 + g(x)g(h))} \right)

M1

lim⁡h→0(g(h)h(1+g(x)g(h)))=lim⁡h→0(g(h)/h(1+g(x)g(h)))=lim⁡h→0(g(h)h)=g′(0)=k\lim_{h \to 0} \left( \frac{g(h)}{h(1 + g(x)g(h))} \right) = \lim_{h \to 0} \left( \frac{g(h)/h}{(1 + g(x)g(h))} \right) = \lim_{h \to 0} \left( \frac{g(h)}{h} \right) = g'(0) = k

M1 A1

Thus g′(x)=k(1−(g(x))2)g'(x) = k(1 - (g(x))^2) A1

34


g′(x)(1−(g(x))2)=k\frac{g'(x)}{(1 - (g(x))^2)} = k

Integrating,

tanh⁡−1(g(x))=kx+c\tanh^{-1}(g(x)) = kx + c

M1

g(x)=tanh⁡(kx+c)g(x) = \tanh(kx + c)

As g(0)=0g(0) = 0, tanh⁡(c)=0\tanh(c) = 0 and so c=0c = 0 M1

Thus

g(x)=tanh⁡(kx)g(x) = \tanh(kx)

A1 [11]

[Alternatively, integrating having used partial fractions,

12ln⁡(1+g(x)1−g(x))=kx+c\frac{1}{2} \ln \left( \frac{1 + g(x)}{1 - g(x)} \right) = kx + c M1

As g(0)=0g(0) = 0, c=0c = 0

1+g(x)1−g(x)=e2kx\frac{1 + g(x)}{1 - g(x)} = e^{2kx} M1

and so

g(x)=e2kx−1e2kx+1g(x) = \frac{e^{2kx} - 1}{e^{2kx} + 1} A1 [3]

35

Model Solution

Part (i)

Showing f(0)=1f(0) = 1:

Set y=0y = 0 in f(x+y)=f(x)f(y)f(x+y) = f(x)f(y):

f(x)=f(x)f(0)for all xf(x) = f(x)f(0) \quad \text{for all } x

f(x)(1−f(0))=0for all xf(x)(1 - f(0)) = 0 \quad \text{for all } x

So either f(x)=0f(x) = 0 for all xx, or f(0)=1f(0) = 1.

If f(x)=0f(x) = 0 for all xx, then f′(x)=0f'(x) = 0 for all xx, contradicting f′(0)=k≠0f'(0) = k \neq 0.

Therefore f(0)=1f(0) = 1.

Showing f′(x)=kf(x)f'(x) = kf(x):

Using the definition (∗)(*):

f′(x)=lim⁡h→0f(x+h)−f(x)hf'(x) = \lim_{h \to 0} \frac{f(x+h) - f(x)}{h}

Applying the functional equation with f(x+h)=f(x)f(h)f(x+h) = f(x)f(h):

f′(x)=lim⁡h→0f(x)f(h)−f(x)h=f(x)lim⁡h→0f(h)−1hf'(x) = \lim_{h \to 0} \frac{f(x)f(h) - f(x)}{h} = f(x) \lim_{h \to 0} \frac{f(h) - 1}{h}

Now, since f(0)=1f(0) = 1:

lim⁡h→0f(h)−1h=lim⁡h→0f(0+h)−f(0)h=f′(0)=k\lim_{h \to 0} \frac{f(h) - 1}{h} = \lim_{h \to 0} \frac{f(0+h) - f(0)}{h} = f'(0) = k

Therefore f′(x)=kf(x)f'(x) = kf(x).

Finding f(x)f(x):

f′(x)f(x)=k\frac{f'(x)}{f(x)} = k

Integrating both sides:

ln⁡f(x)=kx+c\ln f(x) = kx + c

f(x)=Aekxf(x) = Ae^{kx}

Since f(0)=1f(0) = 1: A=1A = 1, so:

f(x)=ekx\boxed{f(x) = e^{kx}}


Part (ii)

Finding g(0)g(0):

Set y=0y = 0 in g(x+y)=g(x)+g(y)1+g(x)g(y)g(x+y) = \dfrac{g(x)+g(y)}{1+g(x)g(y)}:

g(x)=g(x)+g(0)1+g(x)g(0)g(x) = \frac{g(x) + g(0)}{1 + g(x)g(0)}

g(x)(1+g(x)g(0))=g(x)+g(0)g(x)(1 + g(x)g(0)) = g(x) + g(0)

g(x)+g(x)2g(0)=g(x)+g(0)g(x) + g(x)^2 g(0) = g(x) + g(0)

g(0)(g(x)2−1)=0g(0)(g(x)^2 - 1) = 0

Since ∣g(x)∣<1|g(x)| < 1 for all xx, we have g(x)2−1≠0g(x)^2 - 1 \neq 0, so g(0)=0g(0) = 0.

Finding g′(x)g'(x):

g′(x)=lim⁡h→0g(x+h)−g(x)h=lim⁡h→0g(x)+g(h)1+g(x)g(h)−g(x)hg'(x) = \lim_{h \to 0} \frac{g(x+h) - g(x)}{h} = \lim_{h \to 0} \frac{\frac{g(x)+g(h)}{1+g(x)g(h)} - g(x)}{h}

Combining the fraction in the numerator:

=lim⁡h→0g(x)+g(h)−g(x)(1+g(x)g(h))h(1+g(x)g(h))= \lim_{h \to 0} \frac{g(x) + g(h) - g(x)(1 + g(x)g(h))}{h(1 + g(x)g(h))}

=lim⁡h→0g(h)−g(x)2g(h)h(1+g(x)g(h))= \lim_{h \to 0} \frac{g(h) - g(x)^2 g(h)}{h(1 + g(x)g(h))}

=lim⁡h→0g(h)(1−g(x)2)h(1+g(x)g(h))= \lim_{h \to 0} \frac{g(h)(1 - g(x)^2)}{h(1 + g(x)g(h))}

=(1−g(x)2)lim⁡h→0g(h)/h1+g(x)g(h)= (1 - g(x)^2) \lim_{h \to 0} \frac{g(h)/h}{1 + g(x)g(h)}

As h→0h \to 0: g(h)→g(0)=0g(h) \to g(0) = 0, so 1+g(x)g(h)→11 + g(x)g(h) \to 1, and g(h)h→g′(0)=k\dfrac{g(h)}{h} \to g'(0) = k.

g′(x)=k(1−g(x)2)\boxed{g'(x) = k(1 - g(x)^2)}

Finding g(x)g(x):

g′(x)1−g(x)2=k\frac{g'(x)}{1 - g(x)^2} = k

Integrating both sides. Since ∣g(x)∣<1|g(x)| < 1, we use the standard result ∫du1−u2=tanh⁡−1u\displaystyle\int \frac{du}{1-u^2} = \tanh^{-1} u:

tanh⁡−1(g(x))=kx+c\tanh^{-1}(g(x)) = kx + c

With g(0)=0g(0) = 0: tanh⁡−1(0)=0\tanh^{-1}(0) = 0, so c=0c = 0.

g(x)=tanh⁡(kx)\boxed{g(x) = \tanh(kx)}

We can verify: tanh⁡\tanh satisfies the addition formula tanh⁡(x+y)=tanh⁡x+tanh⁡y1+tanh⁡xtanh⁡y\tanh(x+y) = \dfrac{\tanh x + \tanh y}{1 + \tanh x \tanh y}, ∣tanh⁡(kx)∣<1|\tanh(kx)| < 1 for all xx, and ddxtanh⁡(kx)∣x=0=k sech2(0)=k\dfrac{d}{dx}\tanh(kx)\big|_{x=0} = k\,\text{sech}^2(0) = k. All conditions are satisfied.

Examiner Notes

第(i)部分需先证明f(0)=1;第(ii)部分g的函数方程形式类似tanh加法公式,推导g’(x)后需正确积分得到g(x)=tanh(kx)。


Topic: 纯数  |  Difficulty: Challenging  |  Marks: 20

3 The matrix A is given by A=(abcd).\mathbf{A} = \begin{pmatrix} a & b \\ c & d \end{pmatrix}.

(i) You are given that the transformation represented by A has a line L1L_1 of invariant points (so that each point on L1L_1 is transformed to itself). Let (x,y)(x, y) be a point on L1L_1. Show that ((a−1)(d−1)−bc)xy=0((a - 1)(d - 1) - bc)xy = 0.

Show further that (a−1)(d−1)=bc(a - 1)(d - 1) = bc.

What can be said about A if L1L_1 does not pass through the origin?

(ii) By considering the cases b≠0b \neq 0 and b=0b = 0 separately, show that if (a−1)(d−1)=bc(a - 1)(d - 1) = bc then the transformation represented by A has a line of invariant points. You should identify the line in the different cases that arise.

(iii) You are given instead that the transformation represented by A has an invariant line L2L_2 (so that each point on L2L_2 is transformed to a point on L2L_2) and that L2L_2 does not pass through the origin. If L2L_2 has the form y=mx+ky = mx + k, show that (a−1)(d−1)=bc(a - 1)(d - 1) = bc.

Hint

(i) (abcd)(xy)=(xy)⇒ax+by=xcx+dy=y\begin{pmatrix} a & b \\ c & d \end{pmatrix} \begin{pmatrix} x \\ y \end{pmatrix} = \begin{pmatrix} x \\ y \end{pmatrix} \Rightarrow ax + by = x \quad cx + dy = y M1

(a−1)x=−by(a - 1)x = -by

−cx=(d−1)y-cx = (d - 1)y

Thus (a−1)x(d−1)y=bycx(a - 1)x(d - 1)y = bycx, that is (a−1)(d−1)xy−bcxy=0(a - 1)(d - 1)xy - bcxy = 0

So ((a−1)(d−1)−bc)xy=0((a - 1)(d - 1) - bc)xy = 0 M1

Thus ((a−1)(d−1)−bc)=0((a - 1)(d - 1) - bc) = 0 or x=0x = 0 or y=0y = 0 M1

If L1L_1 is x=0x = 0, then both by=0by = 0 and dy=y,∀ydy = y, \forall y

Thus, b=0b = 0 and d=1d = 1, meaning that ((a−1)(d−1)−bc)=0((a - 1)(d - 1) - bc) = 0 E1

Similarly, if L1L_1 is y=0y = 0, then both cx=0cx = 0 and ax=x,∀xax = x, \forall x

Then c=0c = 0 and a=1a = 1, meaning that ((a−1)(d−1)−bc)=0((a - 1)(d - 1) - bc) = 0

In all three cases, (a−1)(d−1)=bc(a - 1)(d - 1) = bc E1

Alternatively,

(abcd)(xy)=(xy)⇒(abcd)(xy)=(1001)(xy)\begin{pmatrix} a & b \\ c & d \end{pmatrix} \begin{pmatrix} x \\ y \end{pmatrix} = \begin{pmatrix} x \\ y \end{pmatrix} \Rightarrow \begin{pmatrix} a & b \\ c & d \end{pmatrix} \begin{pmatrix} x \\ y \end{pmatrix} = \begin{pmatrix} 1 & 0 \\ 0 & 1 \end{pmatrix} \begin{pmatrix} x \\ y \end{pmatrix} M1

So (abcd)(xy)−(1001)(xy)=(00)\begin{pmatrix} a & b \\ c & d \end{pmatrix} \begin{pmatrix} x \\ y \end{pmatrix} - \begin{pmatrix} 1 & 0 \\ 0 & 1 \end{pmatrix} \begin{pmatrix} x \\ y \end{pmatrix} = \begin{pmatrix} 0 \\ 0 \end{pmatrix}

That is (a−1bcd−1)(xy)=(00)\begin{pmatrix} a - 1 & b \\ c & d - 1 \end{pmatrix} \begin{pmatrix} x \\ y \end{pmatrix} = \begin{pmatrix} 0 \\ 0 \end{pmatrix} M1

As this is true for a line of invariant points, it does not have a unique solution and so E1

det(a−1bcd−1)=0det \begin{pmatrix} a - 1 & b \\ c & d - 1 \end{pmatrix} = 0 M1

and so ((a−1)(d−1)−bc)=0((a - 1)(d - 1) - bc) = 0 which implies both ((a−1)(d−1)−bc)xy=0((a - 1)(d - 1) - bc)xy = 0 and (a−1)(d−1)=bc(a - 1)(d - 1) = bc E1

If L1L_1 does not pass through the origin then either L1L_1 is a) y=mx+ky = mx + k with k≠0k \neq 0

or b) x=kx = k with k≠0k \neq 0 E1

For a) (abcd)(xmx+k)=(xmx+k)∀x\begin{pmatrix} a & b \\ c & d \end{pmatrix} \begin{pmatrix} x \\ mx + k \end{pmatrix} = \begin{pmatrix} x \\ mx + k \end{pmatrix} \quad \forall x

Thus ax+b(mx+k)=xax + b(mx + k) = x and cx+d(mx+k)=mx+kcx + d(mx + k) = mx + k

As these apply for all xx, and k≠0k \neq 0, bk=0bk = 0 which implies b=0b = 0 and a+bm=1a + bm = 1 and thus a=1a = 1

Also dk=kdk = k implying d=1d = 1 and c+dm=mc + dm = m which thus gives c=0c = 0 M1

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For b) (abcd)(ky)=(ky)∀y\begin{pmatrix} a & b \\ c & d \end{pmatrix} \begin{pmatrix} k \\ y \end{pmatrix} = \begin{pmatrix} k \\ y \end{pmatrix} \forall y

Thus ak+by=kak + by = k and ck+dy=yck + dy = y

So ak=kak = k implying a=1a = 1 and b=0b = 0 and ck=0ck = 0 implying c=0c = 0 and d=1d = 1 M1

Thus A=I\mathbf{A} = \mathbf{I} A1 [9]

(ii) If (a−1)(d−1)=bc(a - 1)(d - 1) = bc and b≠0b \neq 0

then (abcd)(xy)=(ax+bycx+dy)\begin{pmatrix} a & b \\ c & d \end{pmatrix} \begin{pmatrix} x \\ y \end{pmatrix} = \begin{pmatrix} ax + by \\ cx + dy \end{pmatrix} is an invariant point iff ax+by=xax + by = x and cx+dy=ycx + dy = y M1

That is (a−1)x+by=0(a - 1)x + by = 0, (a−1)(d−1)x+b(d−1)y=0(a - 1)(d - 1)x + b(d - 1)y = 0, bcx+b(d−1)y=0bcx + b(d - 1)y = 0 and so cx+(d−1)y=0cx + (d - 1)y = 0 as required. E1

The line of invariant points is thus (a−1)x+by=0(a - 1)x + by = 0 which is cx+(d−1)y=0cx + (d - 1)y = 0 A1

If (a−1)(d−1)=bc(a - 1)(d - 1) = bc and b=0b = 0 then a=1a = 1 or if a≠1a \neq 1, d=1d = 1

a=1a = 1, (10cd)(xy)=(xcx+dy)\begin{pmatrix} 1 & 0 \\ c & d \end{pmatrix} \begin{pmatrix} x \\ y \end{pmatrix} = \begin{pmatrix} x \\ cx + dy \end{pmatrix} so points on cx+(d−1)y=0cx + (d - 1)y = 0 are invariant. B1

a≠1a \neq 1, (a0c1)(xy)=(axcx+y)\begin{pmatrix} a & 0 \\ c & 1 \end{pmatrix} \begin{pmatrix} x \\ y \end{pmatrix} = \begin{pmatrix} ax \\ cx + y \end{pmatrix} so points on x=0x = 0 are invariant. B1 [5]

(iii) L2L_2 is an invariant line implies (abcd)(xmx+k)=(x′mx′+k)\begin{pmatrix} a & b \\ c & d \end{pmatrix} \begin{pmatrix} x \\ mx + k \end{pmatrix} = \begin{pmatrix} x' \\ mx' + k \end{pmatrix} and as L2L_2 does not pass through the origin k≠0k \neq 0 M1

So ax+b(mx+k)=x′ax + b(mx + k) = x' and cx+d(mx+k)=mx′+kcx + d(mx + k) = mx' + k

As these are true for all xx, true for x=0x = 0 and thus bk=x′bk = x' and dk=mx′+kdk = mx' + k giving

dk=mbk+kdk = mbk + k and as k≠0k \neq 0, d=mb+1d = mb + 1 E1

Similarly, for x=1x = 1 and thus a+b(m+k)=x′′a + b(m + k) = x'' and c+d(m+k)=mx′′+kc + d(m + k) = mx'' + k

So c+d(m+k)=m(a+b(m+k))+kc + d(m + k) = m(a + b(m + k)) + k

c+dm+dk=ma+(m+k)(d−1)+kc + dm + dk = ma + (m + k)(d - 1) + k

c+dm+dk=ma+dm+dk−m−k+kc + dm + dk = ma + dm + dk - m - k + k

c=ma−mc = ma - m E1

So m(a−1)=cm(a - 1) = c and d−1=mbd - 1 = mb

Hence, multiplying these m(a−1)(d−1)=mbcm(a - 1)(d - 1) = mbc E1

Thus, if m≠0m \neq 0, (a−1)(d−1)=bc(a - 1)(d - 1) = bc

If m=0m = 0, (abcd)(xk)=(x′k)\begin{pmatrix} a & b \\ c & d \end{pmatrix} \begin{pmatrix} x \\ k \end{pmatrix} = \begin{pmatrix} x' \\ k \end{pmatrix} giving ax+bk=x′ax + bk = x' and cx+dk=kcx + dk = k E1

As these must be true for all xx, when x=0x = 0, dk=kdk = k giving d=1d = 1 and so for choosing any x≠0x \neq 0, we find c=0c = 0. Thus (a−1)(d−1)=0(a - 1)(d - 1) = 0 and bc=0bc = 0 giving (a−1)(d−1)=bc(a - 1)(d - 1) = bc

E1 [6]

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Model Solution

Part (i)

Let (x,y)(x, y) be a point on L1L_1. Since it is an invariant point, A\mathbf{A} maps (x,y)(x, y) to itself:

(abcd)(xy)=(xy)\begin{pmatrix} a & b \\ c & d \end{pmatrix} \begin{pmatrix} x \\ y \end{pmatrix} = \begin{pmatrix} x \\ y \end{pmatrix}

This gives the two equations:

ax+by=x⇒(a−1)x=−by(1)ax + by = x \qquad \Rightarrow \qquad (a-1)x = -by \qquad \qquad \text{(1)}

cx+dy=y⇒cx=−(d−1)y(2)cx + dy = y \qquad \Rightarrow \qquad cx = -(d-1)y \qquad \qquad \text{(2)}

From (1): (a−1)x=−by(a-1)x = -by. From (2): (d−1)y=−cx(d-1)y = -cx.

Multiplying these two equations:

(a−1)(d−1)xy=(−by)(−cx)=bcxy(a-1)(d-1)xy = (-by)(-cx) = bcxy

((a−1)(d−1)−bc)xy=0((a-1)(d-1) - bc)xy = 0

((a−1)(d−1)−bc)xy=0\boxed{((a-1)(d-1) - bc)xy = 0}

as required. ■\qquad \blacksquare

Showing (a−1)(d−1)=bc(a-1)(d-1) = bc:

The equation ((a−1)(d−1)−bc)xy=0((a-1)(d-1) - bc)xy = 0 holds for every point on L1L_1. Since L1L_1 is a line (not just the origin), it contains infinitely many points. We consider three cases:

Case 1: If there exists a point on L1L_1 with x≠0x \neq 0 and y≠0y \neq 0, then we can divide by xyxy to get (a−1)(d−1)−bc=0(a-1)(d-1) - bc = 0, i.e.\ (a−1)(d−1)=bc(a-1)(d-1) = bc.

Case 2: L1L_1 is the line x=0x = 0 (the yy-axis). Then every point (0,y)(0, y) is invariant. From (1): by=0by = 0 for all yy, giving b=0b = 0. From (2): dy=ydy = y for all yy, giving d=1d = 1. Hence (a−1)(d−1)=(a−1)(0)=0(a-1)(d-1) = (a-1)(0) = 0 and bc=0bc = 0, so (a−1)(d−1)=bc(a-1)(d-1) = bc.

Case 3: L1L_1 is the line y=0y = 0 (the xx-axis). Then every point (x,0)(x, 0) is invariant. From (1): (a−1)x=0(a-1)x = 0 for all xx, giving a=1a = 1. From (2): cx=0cx = 0 for all xx, giving c=0c = 0. Hence (a−1)(d−1)=0(a-1)(d-1) = 0 and bc=0bc = 0, so again (a−1)(d−1)=bc(a-1)(d-1) = bc.

In all cases, (a−1)(d−1)=bc(a-1)(d-1) = bc. ■\qquad \blacksquare

If L1L_1 does not pass through the origin: Suppose L1L_1 is the line y=mx+ky = mx + k with k≠0k \neq 0. Every point (x,mx+k)(x, mx+k) satisfies A(xmx+k)=(xmx+k)\mathbf{A}\binom{x}{mx+k} = \binom{x}{mx+k}, so:

(a−1)x+b(mx+k)=0for all x(a-1)x + b(mx + k) = 0 \qquad \text{for all } x

The constant term gives bk=0bk = 0. Since k≠0k \neq 0, we get b=0b = 0. Then the xx-coefficient gives a−1+bm=0a - 1 + bm = 0, so a=1a = 1.

(d−1)(mx+k)+cx=0for all x(d-1)(mx + k) + cx = 0 \qquad \text{for all } x

The constant term gives (d−1)k=0(d-1)k = 0, so d=1d = 1. The xx-coefficient gives c+(d−1)m=0c + (d-1)m = 0, so c=0c = 0.

Therefore A=I\mathbf{A} = \mathbf{I}. The only matrix with an invariant line not through the origin is the identity matrix.


Part (ii)

Case b≠0b \neq 0: We are given (a−1)(d−1)=bc(a-1)(d-1) = bc. Consider the line (a−1)x+by=0(a-1)x + by = 0, i.e.\ y=−(a−1)bxy = -\frac{(a-1)}{b}x.

For any point (x,y)(x, y) on this line:

  • First component: ax+by=ax+b⋅(−a−1bx)=ax−(a−1)x=xax + by = ax + b \cdot \left(-\frac{a-1}{b}x\right) = ax - (a-1)x = x. ✓
  • Second component: cx+dy=cx−d(a−1)bxcx + dy = cx - \frac{d(a-1)}{b}x. We need this to equal y=−a−1bxy = -\frac{a-1}{b}x, so:

cx−d(a−1)bx=−a−1bxcx - \frac{d(a-1)}{b}x = -\frac{a-1}{b}x

Dividing by xx (for x≠0x \neq 0, and the case x=0x = 0 gives y=0y = 0 which is trivially invariant):

c−d(a−1)b=−a−1bc - \frac{d(a-1)}{b} = -\frac{a-1}{b}

cb−d(a−1)=−(a−1)cb - d(a-1) = -(a-1)

bc=(a−1)(d−1)bc = (a-1)(d-1)

This is precisely our hypothesis. So the line of invariant points is (a−1)x+by=0(a-1)x + by = 0, equivalently cx+(d−1)y=0cx + (d-1)y = 0 (these represent the same line since (a−1)(d−1)=bc(a-1)(d-1) = bc).

Case b=0b = 0: The condition (a−1)(d−1)=bc=0(a-1)(d-1) = bc = 0 means a=1a = 1 or d=1d = 1.

  • Subcase a=1a = 1: A=(10cd)\mathbf{A} = \begin{pmatrix} 1 & 0 \\ c & d \end{pmatrix}. The invariant point equations become 0=00 = 0 and cx+(d−1)y=0cx + (d-1)y = 0. The line of invariant points is cx+(d−1)y=0cx + (d-1)y = 0.

  • Subcase d=1d = 1, a≠1a \neq 1: A=(a0c1)\mathbf{A} = \begin{pmatrix} a & 0 \\ c & 1 \end{pmatrix}. The invariant point equations become (a−1)x=0(a-1)x = 0 and cx=0cx = 0. Since a≠1a \neq 1, we need x=0x = 0 (and cx=0cx = 0 is then automatic). The line of invariant points is x=0x = 0.

In every case, A\mathbf{A} has a line of invariant points. ■\qquad \blacksquare


Part (iii)

L2:y=mx+kL_2: y = mx + k with k≠0k \neq 0 is an invariant line, meaning A\mathbf{A} maps every point on L2L_2 to a (possibly different) point on L2L_2. For any xx, the image of (x,mx+k)(x, mx+k) must be of the form (x′,mx′+k)(x', mx'+k):

ax+b(mx+k)=x′(3)ax + b(mx + k) = x' \qquad \qquad \text{(3)}

cx+d(mx+k)=mx′+k(4)cx + d(mx + k) = mx' + k \qquad \qquad \text{(4)}

Case m≠0m \neq 0: From (3): x′=(a+bm)x+bkx' = (a + bm)x + bk. Substitute into (4):

cx+dmx+dk=m(a+bm)x+mbk+kcx + dmx + dk = m(a + bm)x + mbk + k

(c+dm)x+dk=(ma+m2b)x+mbk+k(c + dm)x + dk = (ma + m^2b)x + mbk + k

Equating constant terms (x=0x = 0):

dk=mbk+kdk = mbk + k

Since k≠0k \neq 0, divide by kk:

d=mb+1⇒d−1=mb(5)d = mb + 1 \qquad \Rightarrow \qquad d - 1 = mb \qquad \qquad \text{(5)}

Equating coefficients of xx:

c+dm=ma+m2bc + dm = ma + m^2b

Using (5), dm=mb2+mdm = mb^2 + m:

c+mb2+m=ma+m2bc + mb^2 + m = ma + m^2b

c=ma−m=m(a−1)(6)c = ma - m = m(a - 1) \qquad \qquad \text{(6)}

Multiplying (5) and (6):

(d−1)⋅m(a−1)=mb⋅c(d-1) \cdot m(a-1) = mb \cdot c

m(a−1)(d−1)=mbcm(a-1)(d-1) = mbc

Since m≠0m \neq 0, divide by mm:

(a−1)(d−1)=bc■\boxed{(a-1)(d-1) = bc} \qquad \blacksquare

Case m=0m = 0: The line is y=ky = k with k≠0k \neq 0. For any (x,k)(x, k), the image is (x′,k)(x', k):

ax+bk=x′(7)ax + bk = x' \qquad \qquad \text{(7)}

cx+dk=k(8)cx + dk = k \qquad \qquad \text{(8)}

From (8), since this must hold for all xx: the coefficient of xx gives c=0c = 0, and the constant term gives dk=kdk = k, so d=1d = 1 (since k≠0k \neq 0).

Therefore (a−1)(d−1)=(a−1)⋅0=0(a-1)(d-1) = (a-1) \cdot 0 = 0 and bc=b⋅0=0bc = b \cdot 0 = 0, giving (a−1)(d−1)=bc(a-1)(d-1) = bc. ■\qquad \blacksquare

Examiner Notes

需区分”不变点”(fixed point)和”不变线”(invariant line)两个概念;b=0时需仔细讨论矩阵的特殊形式;第(iii)部分不变线不过原点的条件是关键。


Topic: 纯数  |  Difficulty: Hard  |  Marks: 20

4 The nnth degree polynomial P(x)\text{P}(x) is said to be reflexive if:

(a) P(x)\text{P}(x) is of the form xn−a1xn−1+a2xn−2−⋯+(−1)nanx^n - a_1x^{n-1} + a_2x^{n-2} - \dots + (-1)^n a_n where n⩾1n \geqslant 1; (b) a1,a2,…,ana_1, a_2, \dots, a_n are real; (c) the nn (not necessarily distinct) roots of the equation P(x)=0\text{P}(x) = 0 are a1,a2,…,ana_1, a_2, \dots, a_n.

(i) Find all reflexive polynomials of degree less than or equal to 3.

(ii) For a reflexive polynomial with n>3n > 3, show that 2a2=−a22−a32−⋯−an2.2a_2 = -a_2^2 - a_3^2 - \dots - a_n^2.

Deduce that, if all the coefficients of a reflexive polynomial of degree nn are integers and an≠0a_n \neq 0, then n⩽3n \leqslant 3.

(iii) Determine all reflexive polynomials with integer coefficients.

Hint

(i) Degree 1, x−a1=0x - a_1 = 0 has root x=a1x = a_1 and so x−a1x - a_1 is reflexive. [B1]

Degree 2, x2−a1x+a2=0x^2 - a_1x + a_2 = 0 has to have roots a1a_1 and a2a_2 to be reflexive.

Thus a12−a1a1+a2=0{a_1}^2 - a_1a_1 + a_2 = 0 (giving a2=0a_2 = 0) and a22−a1a2+a2=0{a_2}^2 - a_1a_2 + a_2 = 0 [M1] which is consistent. Thus, x2−a1xx^2 - a_1x (+ 0) [B1]

a1=a1+a2a_1 = a_1 + a_2 and a2=a1a2a_2 = a_1a_2 giving a2=0a_2 = 0 and consistent for any a1a_1 [M1]

Thus, x2−a1xx^2 - a_1x (+ 0) [B1]

Degree 3, x3−a1x2+a2x−a3=0x^3 - a_1x^2 + a_2x - a_3 = 0

a1=a1+a2+a3a_1 = a_1 + a_2 + a_3

a2=a1a2+a2a3+a3a1a_2 = a_1a_2 + a_2a_3 + a_3a_1

a3=a1a2a3a_3 = a_1a_2a_3 [M1]

The first equation implies that a2+a3=0a_2 + a_3 = 0 [M1] or in other words a2=−a3a_2 = -a_3

This result substituted into the second equation implies that a2=a2a3a_2 = a_2a_3 [M1]

Continuing a2a3−a2=0a_2a_3 - a_2 = 0, a2(a3−1)=0a_2(a_3 - 1) = 0 [M1] so either a2=0a_2 = 0 and thus a3=0a_3 = 0 in which case the equations are consistent for any a1a_1 [M1] or a3=1a_3 = 1 and thus a2=−1a_2 = -1 and a1=−1a_1 = -1 from the third equation. [M1]

Alternatively, from the third equation, a3=a1a2a3a_3 = a_1a_2a_3, a1a2a3−a3=0a_1a_2a_3 - a_3 = 0, a3(a1a2−1)=0a_3(a_1a_2 - 1) = 0

so a3=0a_3 = 0, a2=0a_2 = 0 and consistent for any a1a_1 or a1a2=1a_1a_2 = 1 In the latter case it is simpler to use equation two route again.

Yielding x3−a1x2x^3 - a_1x^2 [A1] or x3+x2−x−1x^3 + x^2 - x - 1 [A1]

Alternative approach a13−a1a12+a2a1−a3=0{a_1}^3 - a_1{a_1}^2 + a_2a_1 - a_3 = 0 (A), a23−a1a22+a2a2−a3=0{a_2}^3 - a_1{a_2}^2 + a_2a_2 - a_3 = 0 (B), and

a33−a1a32+a2a3−a3=0{a_3}^3 - a_1{a_3}^2 + a_2a_3 - a_3 = 0 (C) [M1]

So (A) implies a3=a1a2a_3 = a_1a_2 and thus (B) becomes a23−a1a22+a22−a1a2=0{a_2}^3 - a_1{a_2}^2 + {a_2}^2 - a_1a_2 = 0

Hence a2(a22−a1a2+a2−a1)=a2(a2+1)(a2−a1)=0a_2({a_2}^2 - a_1a_2 + a_2 - a_1) = a_2(a_2 + 1)(a_2 - a_1) = 0 [M1]

Therefore, a2=0a_2 = 0 and so from (A) a3=0a_3 = 0 giving the polynomial x3−a1x2x^3 - a_1x^2, which is reflexive [A1]

or a2=−1a_2 = -1 and so from (A) a3=−a1a_3 = -a_1 giving the polynomial

38


x3−a1x2−x+a1=(x−a1)(x2−1)x^3 - a_1x^2 - x + a_1 = (x - a_1)(x^2 - 1) for which the equation has roots a1a_1 and ±1\pm 1. Thus a3=−a1=1a_3 = -a_1 = 1 so the polynomial is x3+x2−x−1x^3 + x^2 - x - 1 for which the equation has roots −1-1, −1-1 and 11 and so is reflexive M1 A1

or a2=a1a_2 = a_1 and so A gives a3=a12a_3 = {a_1}^2 But C is a33−a1a32+a2a3−a3=0{a_3}^3 - a_1{a_3}^2 + a_2a_3 - a_3 = 0 and so

a3(a32−a1a3+a1−a3)=0a_3({a_3}^2 - a_1a_3 + a_1 - a_3) = 0, a3(a3−a1)(a3−1)=0a_3(a_3 - a_1)(a_3 - 1) = 0 M1

a3=0a_3 = 0, a1=0a_1 = 0, a2=0a_2 = 0 giving the reflexive polynomial x3x^3

a3=a1a_3 = a_1, implies a1=0a_1 = 0 or a1=1a_1 = 1 giving x3x^3 again or a1=a2=a3=1a_1 = a_2 = a_3 = 1 giving the polynomial x3−x2+x−1=(x2+1)(x−1)x^3 - x^2 + x - 1 = (x^2 + 1)(x - 1) which is not reflexive. E1

a3=1a_3 = 1, implies a1=a2=±1a_1 = a_2 = \pm 1 giving 1,1,1 which is not possible or -1,-1,1 (both already considered) E1 [11]

Summary degree 1 x−a1x - a_1, degree 2 x2−a1xx^2 - a_1x (+ 0), and degree 3 x3−a1x2x^3 - a_1x^2 or x3+x2−x−1x^3 + x^2 - x - 1

(ii)

a1=∑r=1nara_1 = \sum_{r=1}^{n} a_r

and so,

∑r=2nar=0\sum_{r=2}^{n} a_r = 0

B1

a2=12∑i≠jaiaja_2 = \frac{1}{2} \sum_{i \neq j} a_i a_j

(∑r=2nar)2=∑r=2nar2+∑i≠jaiaj−2a1∑r=2nar\left( \sum_{r=2}^{n} a_r \right)^2 = \sum_{r=2}^{n} {a_r}^2 + \sum_{i \neq j} a_i a_j - 2a_1 \sum_{r=2}^{n} a_r

M1

Thus

0=∑r=2nar2+2a20 = \sum_{r=2}^{n} {a_r}^2 + 2a_2

Hence

2a2=−a22−a32−⋯−an22a_2 = -{a_2}^2 - {a_3}^2 - \dots - {a_n}^2

as required. A1*

a22+2a2+1=1−a32−⋯−an2{a_2}^2 + 2a_2 + 1 = 1 - {a_3}^2 - \dots - {a_n}^2

Thus,

39


1−a32−⋯−an2≥01 - {a_3}^2 - \dots - {a_n}^2 \ge 0

So

a32+⋯+an2≤1{a_3}^2 + \dots + {a_n}^2 \le 1

M1

If all the coefficients are integers, then as an≠0a_n \neq 0, an2=1{a_n}^2 = 1 and the other coefficients for

r=3,…,n−1r = 3, \dots, n - 1 are zero. But

an=∏r=1nara_n = \prod_{r=1}^n a_r

so we have established a contradiction. Thus if an≠0a_n \neq 0, n≤3n \le 3 E1 [5]

(iii) So apart from those found in (i) with a1a_1 integer, any other reflexive polynomials must have an=0a_n = 0 E1

So

xn−a1xn−1+a2xn−2−⋯+(−1)n−1an−1x=0x^n - a_1 x^{n-1} + a_2 x^{n-2} - \dots + (-1)^{n-1} a_{n-1} x = 0 ∴x(xn−1−a1xn−2+a2xn−3−⋯+(−1)n−1an−1)=0\therefore x(x^{n-1} - a_1 x^{n-2} + a_2 x^{n-3} - \dots + (-1)^{n-1} a_{n-1}) = 0 M1

which gives a root of zero plus the roots of the bracketed expression. Thus we require the bracketed expression to be itself a reflexive polynomial. This can only happen if either the bracketed expression is of degree 3 or, in turn, an−1=0a_{n-1} = 0, and so on. E1

Hence, we have x−a1x - a_1, x2−a1xx^2 - a_1 x (+ 0), x3−a1x2x^3 - a_1 x^2, (with a1a_1 integer), x3+x2−x−1x^3 + x^2 - x - 1, or these multiplied by xrx^r.

That is (x−a1)xr(x - a_1)x^r or (x+1)2(x−1)xr(x + 1)^2(x - 1)x^r with r=0,1,2,…r = 0, 1, 2, \dots A1 [4]

40

Model Solution

Part (i)

Degree 1: P(x)=x−a1\mathrm{P}(x) = x - a_1. The equation x−a1=0x - a_1 = 0 has root x=a1x = a_1. The single coefficient is a1a_1, which equals the single root. So x−a1x - a_1 is reflexive for every real a1a_1.

Degree 2: P(x)=x2−a1x+a2\mathrm{P}(x) = x^2 - a_1 x + a_2. By Vieta’s formulas, the roots a1,a2a_1, a_2 satisfy:

a1+a2=a1⇒a2=0(1)a_1 + a_2 = a_1 \qquad \Rightarrow \qquad a_2 = 0 \qquad \qquad \text{(1)}

a1⋅a2=a2⇒a2(a1−1)=0(2)a_1 \cdot a_2 = a_2 \qquad \Rightarrow \qquad a_2(a_1 - 1) = 0 \qquad \qquad \text{(2)}

From (1), a2=0a_2 = 0, which satisfies (2) for any a1a_1. So the reflexive polynomials of degree 2 are:

x2−a1xfor any real a1\boxed{x^2 - a_1 x \quad \text{for any real } a_1}

Verification: x2−a1x=x(x−a1)x^2 - a_1 x = x(x - a_1) has roots 00 and a1a_1, which are indeed a2=0a_2 = 0 and a1a_1. ✓

Degree 3: P(x)=x3−a1x2+a2x−a3\mathrm{P}(x) = x^3 - a_1 x^2 + a_2 x - a_3. By Vieta’s formulas:

a1+a2+a3=a1⇒a2+a3=0⇒a3=−a2(3)a_1 + a_2 + a_3 = a_1 \qquad \Rightarrow \qquad a_2 + a_3 = 0 \qquad \Rightarrow \qquad a_3 = -a_2 \qquad \qquad \text{(3)}

a1a2+a2a3+a3a1=a2(4)a_1 a_2 + a_2 a_3 + a_3 a_1 = a_2 \qquad \qquad \text{(4)}

a1a2a3=a3⇒a3(a1a2−1)=0(5)a_1 a_2 a_3 = a_3 \qquad \Rightarrow \qquad a_3(a_1 a_2 - 1) = 0 \qquad \qquad \text{(5)}

From (5), either a3=0a_3 = 0 or a1a2=1a_1 a_2 = 1.

Subcase a3=0a_3 = 0: From (3), a2=0a_2 = 0. Equation (4) becomes 0=00 = 0. So a1a_1 is free, giving the polynomial x3−a1x2x^3 - a_1 x^2.

Verification: x3−a1x2=x2(x−a1)x^3 - a_1 x^2 = x^2(x - a_1) has roots 0,0,a10, 0, a_1, which are a2=0a_2 = 0, a3=0a_3 = 0, a1a_1. ✓

Subcase a1a2=1a_1 a_2 = 1, a3≠0a_3 \neq 0: From (3), a3=−a2a_3 = -a_2. Substitute into (4):

a1a2+a2(−a2)+(−a2)a1=a2a_1 a_2 + a_2(-a_2) + (-a_2) a_1 = a_2

a1a2−a22−a1a2=a2a_1 a_2 - a_2^2 - a_1 a_2 = a_2

−a22=a2-a_2^2 = a_2

a2(a2+1)=0a_2(a_2 + 1) = 0

Since a3=−a2≠0a_3 = -a_2 \neq 0, we have a2≠0a_2 \neq 0, so a2=−1a_2 = -1. Then a3=−(−1)=1a_3 = -(-1) = 1 and a1=1a2=−1a_1 = \frac{1}{a_2} = -1.

Verification: P(x)=x3+x2−x−1=(x+1)2(x−1)\mathrm{P}(x) = x^3 + x^2 - x - 1 = (x+1)^2(x-1), with roots −1,−1,1-1, -1, 1. These are a1=−1a_1 = -1, a2=−1a_2 = -1, a3=1a_3 = 1. ✓

So the reflexive polynomials of degree ⩽3\leqslant 3 are:

x−a1,x2−a1x,x3−a1x2(any real a1),x3+x2−x−1\boxed{x - a_1, \quad x^2 - a_1 x, \quad x^3 - a_1 x^2 \quad (\text{any real } a_1), \qquad x^3 + x^2 - x - 1}


Part (ii)

For a reflexive polynomial of degree nn, the roots are a1,a2,…,ana_1, a_2, \ldots, a_n. By Vieta’s formulas:

a1=∑r=1nar⇒∑r=2nar=0(6)a_1 = \sum_{r=1}^{n} a_r \qquad \Rightarrow \qquad \sum_{r=2}^{n} a_r = 0 \qquad \qquad \text{(6)}

a2=∑1⩽i<j⩽naiaj(7)a_2 = \sum_{1 \leqslant i < j \leqslant n} a_i a_j \qquad \qquad \text{(7)}

Consider the square of ∑r=2nar\sum_{r=2}^{n} a_r:

(∑r=2nar)2=∑r=2nar2+2∑2⩽i<j⩽naiaj\left(\sum_{r=2}^{n} a_r\right)^2 = \sum_{r=2}^{n} a_r^2 + 2 \sum_{2 \leqslant i < j \leqslant n} a_i a_j

From (6), the left side is 00, so:

0=∑r=2nar2+2∑2⩽i<j⩽naiaj(8)0 = \sum_{r=2}^{n} a_r^2 + 2 \sum_{2 \leqslant i < j \leqslant n} a_i a_j \qquad \qquad \text{(8)}

Now we relate ∑2⩽i<j⩽naiaj\sum_{2 \leqslant i < j \leqslant n} a_i a_j to a2a_2. From (7):

a2=∑1⩽i<j⩽naiaj=a1∑r=2nar+∑2⩽i<j⩽naiaja_2 = \sum_{1 \leqslant i < j \leqslant n} a_i a_j = a_1 \sum_{r=2}^{n} a_r + \sum_{2 \leqslant i < j \leqslant n} a_i a_j

By (6), a1∑r=2nar=a1⋅0=0a_1 \sum_{r=2}^{n} a_r = a_1 \cdot 0 = 0, so:

a2=∑2⩽i<j⩽naiaja_2 = \sum_{2 \leqslant i < j \leqslant n} a_i a_j

Substituting into (8):

0=∑r=2nar2+2a20 = \sum_{r=2}^{n} a_r^2 + 2a_2

2a2=−∑r=2nar2=−a22−a32−⋯−an22a_2 = -\sum_{r=2}^{n} a_r^2 = -a_2^2 - a_3^2 - \cdots - a_n^2

2a2=−a22−a32−⋯−an2■\boxed{2a_2 = -a_2^2 - a_3^2 - \cdots - a_n^2} \qquad \blacksquare

Deduction: Rearranging:

a22+2a2+a32+⋯+an2=0a_2^2 + 2a_2 + a_3^2 + \cdots + a_n^2 = 0

(a2+1)2+a32+⋯+an2=1(a_2 + 1)^2 + a_3^2 + \cdots + a_n^2 = 1

Since squares are non-negative:

a32+a42+⋯+an2=1−(a2+1)2⩽1a_3^2 + a_4^2 + \cdots + a_n^2 = 1 - (a_2 + 1)^2 \leqslant 1

If all coefficients are integers and an≠0a_n \neq 0, then an2⩾1a_n^2 \geqslant 1. Combined with a32+⋯+an2⩽1a_3^2 + \cdots + a_n^2 \leqslant 1, we must have an2=1a_n^2 = 1 and a3=a4=⋯=an−1=0a_3 = a_4 = \cdots = a_{n-1} = 0.

From (6): a2+an=0a_2 + a_n = 0 (since a3=⋯=an−1=0a_3 = \cdots = a_{n-1} = 0), so a2=−an=∓1a_2 = -a_n = \mp 1.

From a1a2⋯an=ana_1 a_2 \cdots a_n = a_n (the product of roots equals ana_n), dividing by an≠0a_n \neq 0:

a1a2⋯an−1=1a_1 a_2 \cdots a_{n-1} = 1

Since a3=⋯=an−1=0a_3 = \cdots = a_{n-1} = 0 (and n>3n > 3 means at least one such coefficient exists), the left side is 00. But the right side is 11. Contradiction.

Therefore, if all coefficients are integers and an≠0a_n \neq 0, then n⩽3n \leqslant 3. ■\qquad \blacksquare


Part (iii)

From part (ii), any reflexive polynomial with integer coefficients and n>3n > 3 must have an=0a_n = 0. Then:

P(x)=xn−a1xn−1+⋯+(−1)n−1an−1x=x⋅Q(x)\mathrm{P}(x) = x^n - a_1 x^{n-1} + \cdots + (-1)^{n-1} a_{n-1} x = x \cdot \mathrm{Q}(x)

where Q(x)=xn−1−a1xn−2+⋯+(−1)n−1an−1\mathrm{Q}(x) = x^{n-1} - a_1 x^{n-2} + \cdots + (-1)^{n-1} a_{n-1}.

Since P(x)=0\mathrm{P}(x) = 0 has root x=0=anx = 0 = a_n, and the remaining roots are a1,…,an−1a_1, \ldots, a_{n-1}, the polynomial Q(x)\mathrm{Q}(x) must have roots a1,…,an−1a_1, \ldots, a_{n-1}. Moreover, Q(x)\mathrm{Q}(x) has the correct sign alternation (the coefficient of xn−1−kx^{n-1-k} is (−1)kak(-1)^k a_k). So Q(x)\mathrm{Q}(x) is itself reflexive of degree n−1n-1.

By induction, we keep factoring out xx until we reach a reflexive polynomial of degree ⩽3\leqslant 3 with integer coefficients. From part (i), these are:

  • Degree 1: x−a1x - a_1 with a1∈Za_1 \in \mathbb{Z}
  • Degree 2: x2−a1xx^2 - a_1 x with a1∈Za_1 \in \mathbb{Z}
  • Degree 3: x3−a1x2x^3 - a_1 x^2 with a1∈Za_1 \in \mathbb{Z}, or x3+x2−x−1=(x+1)2(x−1)x^3 + x^2 - x - 1 = (x+1)^2(x-1)

But x2−a1x=x(x−a1)x^2 - a_1 x = x(x - a_1) is just xx times a degree-1 reflexive, and x3−a1x2=x2(x−a1)x^3 - a_1 x^2 = x^2(x - a_1) is x2x^2 times a degree-1 reflexive. So the complete list of reflexive polynomials with integer coefficients is:

(x−a1)⋅xror(x+1)2(x−1)⋅xrwith a1∈Z, r=0,1,2,…\boxed{(x - a_1) \cdot x^r \qquad \text{or} \qquad (x+1)^2(x-1) \cdot x^r \qquad \text{with } a_1 \in \mathbb{Z},\ r = 0, 1, 2, \ldots}

Equivalently: xr(x−a1)x^r(x - a_1) for any integer a1a_1 and non-negative integer rr, or xr(x+1)2(x−1)x^r(x+1)^2(x-1) for any non-negative integer rr. ■\qquad \blacksquare

Examiner Notes

此题概念新颖,需仔细理解定义中”系数=根”的含义。第(ii)部分利用平方和>=0推出a2=0,进而限制系数取值。整系数条件下n<=3的证明是关键难点。


Topic: 纯数  |  Difficulty: Hard  |  Marks: 20

5 (i) Let f(x)=xx2+p,f(x) = \frac{x}{\sqrt{x^2 + p}}, where pp is a non-zero constant. Sketch the curve y=f(x)y = f(x) for x⩾0x \geqslant 0 in the case p>0p > 0.

(ii) Let I=∫1(b2−y2)c2−y2 dy,I = \int \frac{1}{(b^2 - y^2)\sqrt{c^2 - y^2}} \, dy, where bb and cc are positive constants. Use the substitution y=bxx2+py = \frac{bx}{\sqrt{x^2 + p}}, where pp is a suitably chosen constant, to show that I=∫1b2+(b2−c2)x2 dx.I = \int \frac{1}{b^2 + (b^2 - c^2)x^2} \, dx. Evaluate ∫121(3−y2)2−y2 dy.\int_1^{\sqrt{2}} \frac{1}{(3 - y^2)\sqrt{2 - y^2}} \, dy. [ Note: ∫1a2+x2 dx=1atan⁡−1xa+ constant.\int \frac{1}{a^2 + x^2} \, dx = \frac{1}{a} \tan^{-1} \frac{x}{a} + \text{ constant.} ]

Hence evaluate ∫121y(3y2−1)2y2−1 dy.\int_{\frac{1}{\sqrt{2}}}^1 \frac{y}{(3y^2 - 1)\sqrt{2y^2 - 1}} \, dy.

(iii) By means of a suitable substitution, evaluate ∫1211(3y2−1)2y2−1 dy.\int_{\frac{1}{\sqrt{2}}}^1 \frac{1}{(3y^2 - 1)\sqrt{2y^2 - 1}} \, dy.

Hint

(i) f(x)=xx2+pf(x) = \frac{x}{\sqrt{x^2 + p}} f′(x)=x2+p−x122xx2+px2+p=p(x2+p)32f'(x) = \frac{\sqrt{x^2 + p} - x \frac{1}{2} \frac{2x}{\sqrt{x^2 + p}}}{x^2 + p} = \frac{p}{(x^2 + p)^{\frac{3}{2}}}

M1

G1

G1

[3]

(ii) for answers using substitution from question paper

y=bxx2+p⇒dydx=bp(x2+p)32y = \frac{bx}{\sqrt{x^2 + p}} \Rightarrow \frac{dy}{dx} = \frac{bp}{(x^2 + p)^{\frac{3}{2}}} b2−y2=b2−b2x2x2+p=(b2−b2)x2+b2px2+p=b2px2+pb^2 - y^2 = b^2 - \frac{b^2x^2}{x^2 + p} = \frac{(b^2 - b^2)x^2 + b^2p}{x^2 + p} = \frac{b^2p}{x^2 + p}

M1

c2−y2=c2−b2x2x2+p=(c2−b2)x2+c2px2+pc^2 - y^2 = c^2 - \frac{b^2x^2}{x^2 + p} = \frac{(c^2 - b^2)x^2 + c^2p}{x^2 + p}

M1

So ∫1(b2−y2)c2−y2 dy=∫(x2+p)b2px2+p[(c2−b2)x2+c2p]bp(x2+p)32 dx\int \frac{1}{(b^2 - y^2)\sqrt{c^2 - y^2}} \, dy = \int \frac{(x^2 + p)}{b^2p} \frac{\sqrt{x^2 + p}}{\sqrt{[(c^2 - b^2)x^2 + c^2p]}} \frac{bp}{(x^2 + p)^{\frac{3}{2}}} \, dx

M1

=∫1b[(c2−b2)x2+c2p] dx= \int \frac{1}{b\sqrt{[(c^2 - b^2)x^2 + c^2p]}} \, dx

41


M1 [4]

Let c2=2c^2 = 2 M1

Let b2=3b^2 = 3 M1

Thus ∫121(3−y2)2−y2 dy=∫??13+x2 dx=[13tan⁡−1(x3)]??\int_1^{\sqrt{2}} \frac{1}{(3 - y^2)\sqrt{2 - y^2}} \, dy = \int_?^? \frac{1}{3 + x^2} \, dx = \left[ \frac{1}{\sqrt{3}} \tan^{-1} \left( \frac{x}{\sqrt{3}} \right) \right]_?^? M1 M1 M1 [5]

Let y=1xy = \frac{1}{x}, dydx=−1x2\frac{dy}{dx} = -\frac{1}{x^2} M1

∫121y(3y2−1)2y2−1 dy=∫211x13x2−112x2−1×−1x2 dx=∫121(3−x2)2−x2 dx\int_{\frac{1}{\sqrt{2}}}^1 \frac{y}{(3y^2 - 1)\sqrt{2y^2 - 1}} \, dy = \int_{\sqrt{2}}^1 \frac{1}{x} \frac{1}{\frac{3}{x^2} - 1} \frac{1}{\sqrt{\frac{2}{x^2} - 1}} \times -\frac{1}{x^2} \, dx = \int_1^{\sqrt{2}} \frac{1}{(3 - x^2)\sqrt{2 - x^2}} \, dx M1

and so is same answer as previous part A1 ft [3]

(ii) for answers using correct substitution where candidates have realised there is a misprint

y=cxx2+p⇒dydx=cp(x2+p)32y = \frac{cx}{\sqrt{x^2 + p}} \Rightarrow \frac{dy}{dx} = \frac{cp}{(x^2 + p)^{\frac{3}{2}}}

b2−y2=b2−c2x2x2+p=(b2−c2)x2+b2px2+pb^2 - y^2 = b^2 - \frac{c^2x^2}{x^2 + p} = \frac{(b^2 - c^2)x^2 + b^2p}{x^2 + p}

c2−y2=c2−c2x2x2+p=c2px2+pc^2 - y^2 = c^2 - \frac{c^2x^2}{x^2 + p} = \frac{c^2p}{x^2 + p}

M1

Choose p=1p = 1 B1

So ∫1(b2−y2)c2−y2 dy=∫x2+1b2+(b2−c2)x2x2+1cc(x2+1)32 dx\int \frac{1}{(b^2 - y^2)\sqrt{c^2 - y^2}} \, dy = \int \frac{x^2 + 1}{b^2 + (b^2 - c^2)x^2} \frac{\sqrt{x^2 + 1}}{c} \frac{c}{(x^2 + 1)^{\frac{3}{2}}} \, dx M1

=∫1b2+(b2−c2)x2 dx= \int \frac{1}{b^2 + (b^2 - c^2)x^2} \, dx A1* [4]

42


Let c2=2c^2 = 2 Then (x2+1)y2=2x2(x^2 + 1)y^2 = 2x^2 so x2=y22−y2x^2 = \frac{y^2}{2-y^2} and when y=1,x=1y = 1, x = 1

and y→2,x→∞y \rightarrow \sqrt{2}, x \rightarrow \infty

Let b2=3b^2 = 3 [B1 M1 A1]

Thus

∫121(3−y2)2−y2dy=∫1∞13+x2dx=[13tan⁡−1(x3)]1∞=13(π2−π6)=π33\int_{1}^{\sqrt{2}} \frac{1}{(3 - y^2)\sqrt{2 - y^2}} dy = \int_{1}^{\infty} \frac{1}{3 + x^2} dx = \left[ \frac{1}{\sqrt{3}} \tan^{-1} \left( \frac{x}{\sqrt{3}} \right) \right]_{1}^{\infty} = \frac{1}{\sqrt{3}} \left( \frac{\pi}{2} - \frac{\pi}{6} \right) = \frac{\pi}{3\sqrt{3}}

[M1 A1] [5]

Let y=1x,dydx=−1x2y = \frac{1}{x}, \frac{dy}{dx} = -\frac{1}{x^2} [M1]

∫121y(3y2−1)2y2−1dy=∫211x3x2−112x2−1×−1x2dx=∫121(3−x2)2−x2dx\int_{\frac{1}{\sqrt{2}}}^{1} \frac{y}{(3y^2 - 1)\sqrt{2y^2 - 1}} dy = \int_{\sqrt{2}}^{1} \frac{\frac{1}{x}}{\frac{3}{x^2} - 1} \frac{1}{\sqrt{\frac{2}{x^2} - 1}} \times -\frac{1}{x^2} dx = \int_{1}^{\sqrt{2}} \frac{1}{(3 - x^2)\sqrt{2 - x^2}} dx

[M1]

and so is π33\frac{\pi}{3\sqrt{3}} [A1 ft] [3]

(iii) If

y=bxx2+p⇒dydx=bp(x2+p)32y = \frac{bx}{\sqrt{x^2 + p}} \Rightarrow \frac{dy}{dx} = \frac{bp}{(x^2 + p)^{\frac{3}{2}}}

and so

(x2+p)y2=b2x2,x2=py2b2−y2(x^2 + p)y^2 = b^2x^2, x^2 = \frac{py^2}{b^2 - y^2} [M1]

thus

∫1(3y2−1)2y2−1dy=∫1(3b2x2x2+p−1)2b2x2x2+p−1bp(x2+p)32dx\int \frac{1}{(3y^2 - 1)\sqrt{2y^2 - 1}} dy = \int \frac{1}{\left( \frac{3b^2x^2}{x^2 + p} - 1 \right) \sqrt{\frac{2b^2x^2}{x^2 + p} - 1}} \frac{bp}{(x^2 + p)^{\frac{3}{2}}} dx

=∫bp(3b2x2−(x2+p))2b2x2−(x2+p)dx= \int \frac{bp}{(3b^2x^2 - (x^2 + p)) \sqrt{2b^2x^2 - (x^2 + p)}} dx

[M1]

Choosing 2b2=12b^2 = 1 and p=−1p = -1 we have [B1]

∫1211(3y2−1)2y2−1dy=∫∞2−1212x2+1dx=2∫2∞1x2+2dx\int_{\frac{1}{\sqrt{2}}}^{1} \frac{1}{(3y^2 - 1)\sqrt{2y^2 - 1}} dy = \int_{\infty}^{\sqrt{2}} \frac{-\frac{1}{\sqrt{2}}}{\frac{1}{2}x^2 + 1} dx = \sqrt{2} \int_{\sqrt{2}}^{\infty} \frac{1}{x^2 + 2} dx

43


M1

=2[12tan⁡−1(x2)]2∞=π4= \sqrt{2} \left[ \frac{1}{\sqrt{2}} \tan^{-1} \left( \frac{x}{\sqrt{2}} \right) \right]_{\sqrt{2}}^{\infty} = \frac{\pi}{4}

A1 [5]

Model Solution

Part (i)

We have f(x)=xx2+pf(x) = \dfrac{x}{\sqrt{x^2 + p}} with p>0p > 0.

At x=0x = 0: f(0)=0f(0) = 0.

As x→∞x \to \infty: f(x)=xx2+p=11+p/x2→1−f(x) = \dfrac{x}{\sqrt{x^2+p}} = \dfrac{1}{\sqrt{1+p/x^2}} \to 1^-.

Differentiating: f′(x)=x2+p−x⋅xx2+px2+p=(x2+p)−x2(x2+p)3/2=p(x2+p)3/2f'(x) = \frac{\sqrt{x^2+p} - x \cdot \dfrac{x}{\sqrt{x^2+p}}}{x^2+p} = \frac{(x^2+p) - x^2}{(x^2+p)^{3/2}} = \frac{p}{(x^2+p)^{3/2}}

Since p>0p > 0, f′(x)>0f'(x) > 0 for all x⩾0x \geqslant 0, so ff is strictly increasing.

We can also note that for x>0x > 0: f′′(x)=−3px(x2+p)5/2<0f''(x) = \frac{-3px}{(x^2+p)^{5/2}} < 0

so the curve is concave (curving towards the asymptote from below).

The sketch shows the curve passing through the origin, increasing monotonically, and approaching the horizontal asymptote y=1y = 1 from below. The curve is concave throughout x>0x > 0.


Part (ii)

Note: The question paper contains a misprint. The substitution should be y=cxx2+py = \dfrac{cx}{\sqrt{x^2+p}} (with cc not bb). We use the corrected substitution.

We use y=cxx2+py = \dfrac{cx}{\sqrt{x^2+p}} where pp is to be determined.

Computing dydx\dfrac{dy}{dx}: dydx=cx2+p−cx⋅xx2+px2+p=c(x2+p)−cx2(x2+p)3/2=cp(x2+p)3/2\frac{dy}{dx} = \frac{c\sqrt{x^2+p} - cx \cdot \dfrac{x}{\sqrt{x^2+p}}}{x^2+p} = \frac{c(x^2+p) - cx^2}{(x^2+p)^{3/2}} = \frac{cp}{(x^2+p)^{3/2}}

Computing b2−y2b^2 - y^2: b2−y2=b2−c2x2x2+p=b2(x2+p)−c2x2x2+p=b2p+(b2−c2)x2x2+pb^2 - y^2 = b^2 - \frac{c^2x^2}{x^2+p} = \frac{b^2(x^2+p) - c^2x^2}{x^2+p} = \frac{b^2p + (b^2-c^2)x^2}{x^2+p}

Computing c2−y2c^2 - y^2: c2−y2=c2−c2x2x2+p=c2(x2+p)−c2x2x2+p=c2px2+pc^2 - y^2 = c^2 - \frac{c^2x^2}{x^2+p} = \frac{c^2(x^2+p) - c^2x^2}{x^2+p} = \frac{c^2p}{x^2+p}

So c2−y2=cpx2+p\sqrt{c^2-y^2} = \dfrac{c\sqrt{p}}{\sqrt{x^2+p}}.

Substituting into the integral: I=∫1(b2−y2)c2−y2 dy=∫x2+pb2p+(b2−c2)x2⋅x2+pcp⋅cp(x2+p)3/2 dxI = \int \frac{1}{(b^2-y^2)\sqrt{c^2-y^2}} \, dy = \int \frac{x^2+p}{b^2p+(b^2-c^2)x^2} \cdot \frac{\sqrt{x^2+p}}{c\sqrt{p}} \cdot \frac{cp}{(x^2+p)^{3/2}} \, dx

Simplifying the factors: I=∫cp⋅(x2+p)3/2[b2p+(b2−c2)x2]⋅cp⋅(x2+p)3/2 dx=∫pb2p+(b2−c2)x2 dxI = \int \frac{cp \cdot (x^2+p)^{3/2}}{[b^2p+(b^2-c^2)x^2] \cdot c\sqrt{p} \cdot (x^2+p)^{3/2}} \, dx = \int \frac{\sqrt{p}}{b^2p + (b^2-c^2)x^2} \, dx

For this to equal ∫1b2+(b2−c2)x2 dx\displaystyle\int \frac{1}{b^2 + (b^2-c^2)x^2} \, dx, we choose p=1p = 1:

I=∫1b2+(b2−c2)x2 dxI = \int \frac{1}{b^2 + (b^2-c^2)x^2} \, dx

as required. ■\qquad \blacksquare

Evaluating the specific integral:

With b2=3b^2 = 3 and c2=2c^2 = 2, we have b2−c2=1b^2 - c^2 = 1, and the substitution is y=2 xx2+1y = \dfrac{\sqrt{2}\,x}{\sqrt{x^2+1}}.

From this: y2(x2+1)=2x2y^2(x^2+1) = 2x^2, giving x2=y22−y2x^2 = \dfrac{y^2}{2-y^2}.

When y=1y = 1: x2=1x^2 = 1, so x=1x = 1.

When y=2y = \sqrt{2}: x2→∞x^2 \to \infty, so x→∞x \to \infty.

Therefore: ∫121(3−y2)2−y2 dy=∫1∞13+x2 dx\int_1^{\sqrt{2}} \frac{1}{(3-y^2)\sqrt{2-y^2}} \, dy = \int_1^{\infty} \frac{1}{3+x^2} \, dx

Using the given formula with a=3a = \sqrt{3}: =[13tan⁡−1x3]1∞=13(π2−tan⁡−113)=13(π2−π6)=13⋅π3=π33= \left[\frac{1}{\sqrt{3}}\tan^{-1}\frac{x}{\sqrt{3}}\right]_1^{\infty} = \frac{1}{\sqrt{3}}\left(\frac{\pi}{2} - \tan^{-1}\frac{1}{\sqrt{3}}\right) = \frac{1}{\sqrt{3}}\left(\frac{\pi}{2} - \frac{\pi}{6}\right) = \frac{1}{\sqrt{3}} \cdot \frac{\pi}{3} = \frac{\pi}{3\sqrt{3}}

Hence evaluating the second integral:

Consider the substitution y=1xy = \dfrac{1}{x}, so dy=−1x2 dxdy = -\dfrac{1}{x^2}\,dx.

When y=12y = \dfrac{1}{\sqrt{2}}: x=2x = \sqrt{2}. When y=1y = 1: x=1x = 1.

Transforming the integrand: y(3y2−1)2y2−1=1/x(3/x2−1)2/x2−1\frac{y}{(3y^2-1)\sqrt{2y^2-1}} = \frac{1/x}{(3/x^2-1)\sqrt{2/x^2-1}}

=1/x3−x2x2⋅2−x2x=1/x⋅x3(3−x2)2−x2=x2(3−x2)2−x2= \frac{1/x}{\dfrac{3-x^2}{x^2} \cdot \dfrac{\sqrt{2-x^2}}{x}} = \frac{1/x \cdot x^3}{(3-x^2)\sqrt{2-x^2}} = \frac{x^2}{(3-x^2)\sqrt{2-x^2}}

So: ∫1/21y(3y2−1)2y2−1 dy=∫21x2(3−x2)2−x2⋅(−1x2)dx=∫121(3−x2)2−x2 dx\int_{1/\sqrt{2}}^1 \frac{y}{(3y^2-1)\sqrt{2y^2-1}} \, dy = \int_{\sqrt{2}}^1 \frac{x^2}{(3-x^2)\sqrt{2-x^2}} \cdot \left(-\frac{1}{x^2}\right) dx = \int_1^{\sqrt{2}} \frac{1}{(3-x^2)\sqrt{2-x^2}} \, dx

This is identical to the integral evaluated above, so:

∫1/21y(3y2−1)2y2−1 dy=π33\int_{1/\sqrt{2}}^1 \frac{y}{(3y^2-1)\sqrt{2y^2-1}} \, dy = \frac{\pi}{3\sqrt{3}}


Part (iii)

We evaluate ∫1/211(3y2−1)2y2−1 dy\displaystyle\int_{1/\sqrt{2}}^1 \frac{1}{(3y^2-1)\sqrt{2y^2-1}} \, dy.

The integrand involves y2y^2 throughout (no yy in the numerator), so the substitution y=1/xy = 1/x from part (ii) does not reduce it to the same form. Instead we use y=bxx2+py = \dfrac{bx}{\sqrt{x^2+p}} with suitably chosen bb and pp.

With y=bxx2+py = \dfrac{bx}{\sqrt{x^2+p}}: y2=b2x2x2+py^2 = \frac{b^2x^2}{x^2+p}

3y2−1=3b2x2−(x2+p)x2+p=(3b2−1)x2−px2+p3y^2 - 1 = \frac{3b^2x^2 - (x^2+p)}{x^2+p} = \frac{(3b^2-1)x^2 - p}{x^2+p}

2y2−1=2b2x2−(x2+p)x2+p=(2b2−1)x2−px2+p2y^2 - 1 = \frac{2b^2x^2 - (x^2+p)}{x^2+p} = \frac{(2b^2-1)x^2 - p}{x^2+p}

dydx=bp(x2+p)3/2\frac{dy}{dx} = \frac{bp}{(x^2+p)^{3/2}}

The integral becomes: ∫x2+p(3b2−1)x2−p⋅x2+p(2b2−1)x2−p⋅bp(x2+p)3/2 dx=∫bp[(3b2−1)x2−p](2b2−1)x2−p dx\int \frac{x^2+p}{(3b^2-1)x^2 - p} \cdot \frac{\sqrt{x^2+p}}{\sqrt{(2b^2-1)x^2-p}} \cdot \frac{bp}{(x^2+p)^{3/2}} \, dx = \int \frac{bp}{[(3b^2-1)x^2 - p]\sqrt{(2b^2-1)x^2 - p}} \, dx

We choose 2b2−1=02b^2 - 1 = 0, i.e., b2=12b^2 = \dfrac{1}{2}, b=12b = \dfrac{1}{\sqrt{2}}, and p=−1p = -1.

Then:

  • bp=12⋅(−1)=−12bp = \dfrac{1}{\sqrt{2}} \cdot (-1) = -\dfrac{1}{\sqrt{2}}
  • (3b2−1)x2−p=12x2+1=x2+22(3b^2-1)x^2 - p = \dfrac{1}{2}x^2 + 1 = \dfrac{x^2+2}{2}
  • (2b2−1)x2−p=0+1=1(2b^2-1)x^2 - p = 0 + 1 = 1

The integral simplifies to: ∫−1/2x2+22⋅1 dx=∫−2x2+2 dx\int \frac{-1/\sqrt{2}}{\dfrac{x^2+2}{2} \cdot 1} \, dx = \int \frac{-\sqrt{2}}{x^2+2} \, dx

Limits: From y2=x22(x2−1)y^2 = \dfrac{x^2}{2(x^2-1)}, we get x2=2y22y2−1x^2 = \dfrac{2y^2}{2y^2-1}.

When y=1y = 1: x2=2x^2 = 2, so x=2x = \sqrt{2}.

When y=12y = \dfrac{1}{\sqrt{2}}: y2=12y^2 = \dfrac{1}{2}, x2=10+→∞x^2 = \dfrac{1}{0^+} \to \infty.

Therefore: ∫1/211(3y2−1)2y2−1 dy=∫∞2−2x2+2 dx=2∫2∞1x2+2 dx\int_{1/\sqrt{2}}^1 \frac{1}{(3y^2-1)\sqrt{2y^2-1}} \, dy = \int_{\infty}^{\sqrt{2}} \frac{-\sqrt{2}}{x^2+2} \, dx = \sqrt{2}\int_{\sqrt{2}}^{\infty} \frac{1}{x^2+2} \, dx

Using the formula with a=2a = \sqrt{2}: =2[12tan⁡−1x2]2∞=2⋅12(π2−tan⁡−11)=π2−π4=π4= \sqrt{2}\left[\frac{1}{\sqrt{2}}\tan^{-1}\frac{x}{\sqrt{2}}\right]_{\sqrt{2}}^{\infty} = \sqrt{2} \cdot \frac{1}{\sqrt{2}}\left(\frac{\pi}{2} - \tan^{-1} 1\right) = \frac{\pi}{2} - \frac{\pi}{4} = \frac{\pi}{4}

Examiner Notes

注意试卷勘误:第(ii)部分代换中b应改为c。选择合适的p值是解题关键;需正确处理积分限的变换。


Topic: 纯数  |  Difficulty: Challenging  |  Marks: 20

6 The point PP in the Argand diagram is represented by the complex number zz, which satisfies zz∗−az∗−a∗z+aa∗−r2=0.zz^* - az^* - a^*z + aa^* - r^2 = 0. Here, rr is a positive real number and r2≠a∗ar^2 \neq a^*a. By writing ∣z−a∣2|z - a|^2 as (z−a)(z−a)∗(z - a)(z - a)^*, show that the locus of PP is a circle, CC, the radius and the centre of which you should give.

(i) The point QQ is represented by ω\omega, and is related to PP by ω=1z\omega = \frac{1}{z}. Let C′C' be the locus of QQ. Show that C′C' is also a circle, and give its radius and centre.

If CC and C′C' are the same circle, show that (∣a∣2−r2)2=1(|a|^2 - r^2)^2 = 1 and that either aa is real or aa is imaginary. Give sketches to indicate the position of CC in these two cases.

(ii) Suppose instead that the point QQ is represented by ω\omega, where ω=1z∗\omega = \frac{1}{z^*}. If the locus of QQ is CC, is it the case that either aa is real or aa is imaginary?

Hint

∣z−a∣2=(z−a)(z−a)∗=(z−a)(z∗−a∗)=zz∗−az∗−a∗z+aa∗|z - a|^2 = (z - a)(z - a)^* = (z - a)(z^* - a^*) = zz^* - az^* - a^*z + aa^*

M1

So zz satisfies ∣z−a∣2=r2|z - a|^2 = r^2 which means that the locus of P is a circle (C) centre aa and radius rr (which does not pass through the origin as r2≠aa∗r^2 \neq aa^*.) A1 [2]

(i) As w=1zw = \frac{1}{z}, z=1wz = \frac{1}{w} so 1w1w∗−a1w∗−a∗1w+aa∗−r2=0\frac{1}{w} \frac{1}{w^*} - a \frac{1}{w^*} - a^* \frac{1}{w} + aa^* - r^2 = 0

M1

(aa∗−r2)ww∗−aw−a∗w∗+1=0(aa^* - r^2)ww^* - aw - a^*w^* + 1 = 0

ww∗−aaa∗−r2w−a∗aa∗−r2w∗+1aa∗−r2=0ww^* - \frac{a}{aa^* - r^2}w - \frac{a^*}{aa^* - r^2}w^* + \frac{1}{aa^* - r^2} = 0

ww∗−(a∗aa∗−r2)∗w−(a∗aa∗−r2)w∗+(a∗aa∗−r2)(aaa∗−r2)ww^* - \left(\frac{a^*}{aa^* - r^2}\right)^* w - \left(\frac{a^*}{aa^* - r^2}\right)w^* + \left(\frac{a^*}{aa^* - r^2}\right)\left(\frac{a}{aa^* - r^2}\right) =(a∗aa∗−r2)(aaa∗−r2)−1aa∗−r2= \left(\frac{a^*}{aa^* - r^2}\right)\left(\frac{a}{aa^* - r^2}\right) - \frac{1}{aa^* - r^2}

∣w−a∗aa∗−r2∣2=aa∗(aa∗−r2)2−1aa∗−r2=r2(aa∗−r2)2\left|w - \frac{a^*}{aa^* - r^2}\right|^2 = \frac{aa^*}{(aa^* - r^2)^2} - \frac{1}{aa^* - r^2} = \frac{r^2}{(aa^* - r^2)^2}

M1

So C’ is a circle centre a∗aa∗−r2\frac{a^*}{aa^* - r^2} with radius ∣raa∗−r2∣\left|\frac{r}{aa^* - r^2}\right| A1 [3]

If C and C’ are the same circle, then

a=a∗aa∗−r2a = \frac{a^*}{aa^* - r^2}

M1

and

r2=∣raa∗−r2∣2r^2 = \left|\frac{r}{aa^* - r^2}\right|^2

M1

Thus

r2(∣a∣2−r2)2=r2r^2(|a|^2 - r^2)^2 = r^2

and dividing by r2≠0r^2 \neq 0, (∣a∣2−r2)2=1(|a|^2 - r^2)^2 = 1 as required. A1* [3]

So ∣a∣2−r2=±1|a|^2 - r^2 = \pm 1 and the equation equating the centres becomes a=±a∗a = \pm a^* M1

If a=c+dia = c + di, and a=a∗a = a^*, c+di=c−dic + di = c - di implying d=0d = 0 and hence aa is real. M1 A1

G1

If a=c+dia = c + di, and a=−a∗a = -a^*, c+di=−c+dic + di = -c + di implying c=0c = 0 and hence aa is imaginary. M1 A1

G1 [7]

45


(ii) If w=1z∗w = \frac{1}{z^*} then

∣w∗−a∗aa∗−r2∣2=r2(aa∗−r2)2\left| w^* - \frac{a^*}{aa^* - r^2} \right|^2 = \frac{r^2}{(aa^* - r^2)^2}

M1

so

∣w−aaa∗−r2∣2=r2(aa∗−r2)2\left| w - \frac{a}{aa^* - r^2} \right|^2 = \frac{r^2}{(aa^* - r^2)^2}

M1

and thus, as before ∣a∣2−r2=±1|a|^2 - r^2 = \pm 1 but now a=aaa∗−r2a = \frac{a}{aa^* - r^2} A1

So in the case ∣a∣2−r2=+1|a|^2 - r^2 = +1, then any aa with ∣a∣=r2+1|a| = \sqrt{r^2 + 1} is possible; in the case ∣a∣2−r2=−1|a|^2 - r^2 = -1, a=0a = 0 (in which case r=1r = 1) A1

So, it is not the case that aa is either real or imaginary. A1 [5]

46

Model Solution

Main result:

Recall that ∣z−a∣2=(z−a)(z−a)∗=(z−a)(z∗−a∗)=zz∗−az∗−a∗z+aa∗|z-a|^2 = (z-a)(z-a)^* = (z-a)(z^*-a^*) = zz^* - az^* - a^*z + aa^*.

The given equation zz∗−az∗−a∗z+aa∗−r2=0zz^* - az^* - a^*z + aa^* - r^2 = 0 is therefore equivalent to:

∣z−a∣2=r2|z-a|^2 = r^2

This is the equation of a circle CC with centre aa and radius rr.

Since r2≠aa∗=∣a∣2r^2 \neq aa^* = |a|^2, the circle does not pass through the origin. ■\qquad \blacksquare


Part (i)

Since ω=1/z\omega = 1/z, we have z=1/ωz = 1/\omega and z∗=1/ω∗z^* = 1/\omega^*. Substituting into the equation of CC:

1ω⋅1ω∗−a⋅1ω∗−a∗⋅1ω+aa∗−r2=0\frac{1}{\omega} \cdot \frac{1}{\omega^*} - a \cdot \frac{1}{\omega^*} - a^* \cdot \frac{1}{\omega} + aa^* - r^2 = 0

Multiplying through by ωω∗\omega\omega^*:

1−aω−a∗ω∗+(aa∗−r2)ωω∗=01 - a\omega - a^*\omega^* + (aa^* - r^2)\omega\omega^* = 0

Since r2≠aa∗r^2 \neq aa^*, we may divide by (aa∗−r2)(aa^* - r^2):

ωω∗−aaa∗−r2ω−a∗aa∗−r2ω∗+1aa∗−r2=0\omega\omega^* - \frac{a}{aa^* - r^2}\omega - \frac{a^*}{aa^* - r^2}\omega^* + \frac{1}{aa^* - r^2} = 0

Note that aaa∗−r2=(a∗aa∗−r2)∗\dfrac{a}{aa^* - r^2} = \left(\dfrac{a^*}{aa^* - r^2}\right)^* since aa∗−r2aa^* - r^2 is real.

Completing the square: ∣ω−a∗aa∗−r2∣2=∣a∗aa∗−r2∣2−1aa∗−r2=aa∗(aa∗−r2)2−1aa∗−r2\left|\omega - \frac{a^*}{aa^* - r^2}\right|^2 = \left|\frac{a^*}{aa^* - r^2}\right|^2 - \frac{1}{aa^* - r^2} = \frac{aa^*}{(aa^* - r^2)^2} - \frac{1}{aa^* - r^2}

=aa∗−(aa∗−r2)(aa∗−r2)2=r2(aa∗−r2)2= \frac{aa^* - (aa^* - r^2)}{(aa^* - r^2)^2} = \frac{r^2}{(aa^* - r^2)^2}

So C′C' is a circle with centre a∗aa∗−r2\dfrac{a^*}{aa^* - r^2} and radius r∣aa∗−r2∣\dfrac{r}{|aa^* - r^2|}. ■\qquad \blacksquare

If CC and C′C' are the same circle:

The centres must be equal: a=a∗aa∗−r2...(1)a = \frac{a^*}{aa^* - r^2} \qquad \text{...(1)}

The radii must be equal: r2=r2(aa∗−r2)2...(2)r^2 = \frac{r^2}{(aa^* - r^2)^2} \qquad \text{...(2)}

From (2), since r≠0r \neq 0, we divide by r2r^2: (aa∗−r2)2=1  ⟹  (∣a∣2−r2)2=1(aa^* - r^2)^2 = 1 \implies (|a|^2 - r^2)^2 = 1

So ∣a∣2−r2=±1|a|^2 - r^2 = \pm 1.

Case 1: ∣a∣2−r2=1|a|^2 - r^2 = 1

From (1): a=a∗1=a∗a = \dfrac{a^*}{1} = a^*.

Writing a=c+dia = c + di: c+di=c−dic + di = c - di, so d=0d = 0 and aa is real.

Case 2: ∣a∣2−r2=−1|a|^2 - r^2 = -1

From (1): a=a∗−1=−a∗a = \dfrac{a^*}{-1} = -a^*.

Writing a=c+dia = c + di: c+di=−c+dic + di = -c + di, so c=0c = 0 and aa is imaginary.

Sketches:

  • When aa is real (Case 1): ∣a∣2=r2+1|a|^2 = r^2 + 1, so ∣a∣>r|a| > r. The circle CC is centred on the real axis at aa with radius r<∣a∣r < |a|, so it does not enclose the origin.

  • When aa is imaginary (Case 2): ∣a∣2=r2−1|a|^2 = r^2 - 1, so r>∣a∣r > |a|. The circle CC is centred on the imaginary axis at aa with radius r>∣a∣r > |a|, so it encloses the origin.


Part (ii)

Now ω=1/z∗\omega = 1/z^*, so z∗=1/ωz^* = 1/\omega and z=1/ω∗z = 1/\omega^*. Substituting:

1ω∗⋅1ω−a⋅1ω−a∗⋅1ω∗+aa∗−r2=0\frac{1}{\omega^*} \cdot \frac{1}{\omega} - a \cdot \frac{1}{\omega} - a^* \cdot \frac{1}{\omega^*} + aa^* - r^2 = 0

Multiplying by ωω∗\omega\omega^*: 1−aω∗−a∗ω+(aa∗−r2)ωω∗=01 - a\omega^* - a^*\omega + (aa^* - r^2)\omega\omega^* = 0

Dividing by (aa∗−r2)(aa^* - r^2): ωω∗−a∗aa∗−r2ω−aaa∗−r2ω∗+1aa∗−r2=0\omega\omega^* - \frac{a^*}{aa^* - r^2}\omega - \frac{a}{aa^* - r^2}\omega^* + \frac{1}{aa^* - r^2} = 0

Completing the square: ∣ω−aaa∗−r2∣2=∣a∣2(aa∗−r2)2−1aa∗−r2=∣a∣2−(aa∗−r2)(aa∗−r2)2=r2(aa∗−r2)2\left|\omega - \frac{a}{aa^* - r^2}\right|^2 = \frac{|a|^2}{(aa^* - r^2)^2} - \frac{1}{aa^* - r^2} = \frac{|a|^2 - (aa^* - r^2)}{(aa^* - r^2)^2} = \frac{r^2}{(aa^* - r^2)^2}

So the locus of QQ is a circle with centre a∣a∣2−r2\dfrac{a}{|a|^2 - r^2} and radius r∣∣a∣2−r2∣\dfrac{r}{\bigl||a|^2 - r^2\bigr|}.

If this is to be the circle CC:

Centre: a=a∣a∣2−r2a = \dfrac{a}{|a|^2 - r^2}, which gives ∣a∣2−r2=1|a|^2 - r^2 = 1 (since a≠0a \neq 0).

Radius: r2=r2(∣a∣2−r2)2r^2 = \dfrac{r^2}{(|a|^2 - r^2)^2}, which gives (∣a∣2−r2)2=1(|a|^2 - r^2)^2 = 1.

These are consistent: ∣a∣2−r2=1|a|^2 - r^2 = 1 satisfies (∣a∣2−r2)2=1(|a|^2 - r^2)^2 = 1.

But the centre condition a=a∣a∣2−r2a = \dfrac{a}{|a|^2 - r^2} reduces to ∣a∣2−r2=1|a|^2 - r^2 = 1, which places no constraint on the argument of aa. Any complex number with ∣a∣2=r2+1|a|^2 = r^2 + 1 works.

For example, a=1+ia = 1 + i with r=1r = 1 gives ∣a∣2=2=r2+1|a|^2 = 2 = r^2 + 1. The circle CC has centre 1+i1 + i and radius 11. Since ∣a∣2−r2=1|a|^2 - r^2 = 1, the transformed circle C′C' also has centre 1+i1=1+i\dfrac{1+i}{1} = 1 + i and radius 11=1\dfrac{1}{1} = 1, so C′=CC' = C. But a=1+ia = 1 + i is neither real nor imaginary.

Therefore, it is not the case that either aa is real or aa is imaginary. ■\qquad \blacksquare

Examiner Notes

需注意条件r^2!=aa的几何含义;反演变换将圆映射为圆(或直线)是经典结论;第(ii)部分omega=1/z的情况结论与(i)不同,需独立分析。


Topic: 纯数  |  Difficulty: Challenging  |  Marks: 20

7 The Devil’s Curve is given by y2(y2−b2)=x2(x2−a2),y^2(y^2 - b^2) = x^2(x^2 - a^2), where aa and bb are positive constants.

(i) In the case a=ba = b, sketch the Devil’s Curve.

(ii) Now consider the case a=2a = 2 and b=5b = \sqrt{5}, and x⩾0,y⩾0x \geqslant 0, y \geqslant 0.

(a) Show by considering a quadratic equation in x2x^2 that either 0⩽y⩽10 \leqslant y \leqslant 1 or y⩾2y \geqslant 2.

(b) Describe the curve very close to and very far from the origin.

(c) Find the points at which the tangent to the curve is parallel to the xx-axis and the point at which the tangent to the curve is parallel to the yy-axis.

Sketch the Devil’s Curve in this case.

(iii) Sketch the Devil’s Curve in the case a=2a = 2 and b=5b = \sqrt{5} again, but with −∞<x<∞-\infty < x < \infty and −∞<y<∞-\infty < y < \infty.

Hint

(i) y2(y2−a2)=x2(x2−a2)y^2(y^2 - a^2) = x^2(x^2 - a^2) y4−a2y2+a44=x4−a2x2+a44y^4 - a^2y^2 + \frac{a^4}{4} = x^4 - a^2x^2 + \frac{a^4}{4}

M1

(y2−a22)2=(x2−a22)2\left(y^2 - \frac{a^2}{2}\right)^2 = \left(x^2 - \frac{a^2}{2}\right)^2 y2−a22=±(x2−a22)y^2 - \frac{a^2}{2} = \pm \left(x^2 - \frac{a^2}{2}\right)

So x2=y2x^2 = y^2 which gives y=±xy = \pm x or x2+y2=a2x^2 + y^2 = a^2

A1

Alternatively

y4−x4=a2y2−a2x2y^4 - x^4 = a^2y^2 - a^2x^2 so (y2−x2)(y2+x2)−a2(y2−x2)=0(y^2 - x^2)(y^2 + x^2) - a^2(y^2 - x^2) = 0

M1

G1 [3]

(ii) y2(y2−5)=x2(x2−4)y^2(y^2 - 5) = x^2(x^2 - 4)

a) (x2)2−4x2−y2(y2−5)=0(x^2)^2 - 4x^2 - y^2(y^2 - 5) = 0

So for real x2x^2, 16+4y2(y2−5)≥016 + 4y^2(y^2 - 5) \geq 0

47


M1

(y2)2−5y2+4≥0(y^2)^2 - 5y^2 + 4 \ge 0 (y2−1)(y2−4)≥0(y^2 - 1)(y^2 - 4) \ge 0 (y−1)(y+1)(y−2)(y+2)≥0(y - 1)(y + 1)(y - 2)(y + 2) \ge 0

M1

As y≥0y \ge 0,

(y−1)(y−2)≥0(y - 1)(y - 2) \ge 0

So 0≤y≤10 \le y \le 1 or y≥2y \ge 2 A1* [3]

b) For small x and y,

y4−5y2=x4−4x2y^4 - 5y^2 = x^4 - 4x^2 becomes 5y2≈4x25y^2 \approx 4x^2 so y≈±2x5y \approx \pm \frac{2x}{\sqrt{5}} B1

For large x and y,

y4−5y2=x4−4x2y^4 - 5y^2 = x^4 - 4x^2 becomes y4≈x4y^4 \approx x^4 so y≈±xy \approx \pm x B1 [2]

c)

y2(y2−5)=x2(x2−4)y^2(y^2 - 5) = x^2(x^2 - 4)

(4y3−10y)dydx=4x3−8x(4y^3 - 10y) \frac{dy}{dx} = 4x^3 - 8x

M1

dydx=0⇒4x3−8x=0\frac{dy}{dx} = 0 \Rightarrow 4x^3 - 8x = 0

4x(x2−2)=04x(x^2 - 2) = 0

M1

So x=0x = 0, y=0,5y = 0, \sqrt{5} or x=2x = \sqrt{2}, y=1,2y = 1, 2

Thus (0,5),(2,1),(2,2)(0, \sqrt{5}), (\sqrt{2}, 1), (\sqrt{2}, 2) but not (0,0)(0, 0) A1 B1

dxdy=0⇒4y3−10y=0\frac{dx}{dy} = 0 \Rightarrow 4y^3 - 10y = 0 2y(2y2−5)=02y(2y^2 - 5) = 0

M1

So y=0y = 0, x=0,2x = 0, 2 but y=52y = \sqrt{\frac{5}{2}} gives xx complex E1

Thus (2,0)(2, 0) but not (0,0)(0, 0) A1 [7]

Sketch key points: (0,0)(0,0), (2,2)(\sqrt{2},\sqrt{2}), and (2,0)(2,0). The point with y=1y=1 should be included on the appropriate branch.

[G1 G1 G1 G1] [4]

(iii) Sketch the transformed curve, indicating the same intercepts and the corresponding branch behaviour clearly. [G1 ft] [1]

Model Solution

Part (i)

When a=ba = b, the equation becomes

y2(y2−a2)=x2(x2−a2).y^2(y^2 - a^2) = x^2(x^2 - a^2).

Expanding both sides:

y4−a2y2=x4−a2x2.y^4 - a^2 y^2 = x^4 - a^2 x^2.

Rearranging:

y4−x4=a2(y2−x2).y^4 - x^4 = a^2(y^2 - x^2).

Factorising the left side as a difference of squares:

(y2−x2)(y2+x2)=a2(y2−x2).(y^2 - x^2)(y^2 + x^2) = a^2(y^2 - x^2).

(y2−x2)(y2+x2−a2)=0.(y^2 - x^2)\bigl(y^2 + x^2 - a^2\bigr) = 0.

This gives two factors:

  • y2−x2=0y^2 - x^2 = 0, i.e.\ y=±xy = \pm x (a pair of straight lines through the origin), or
  • x2+y2=a2x^2 + y^2 = a^2 (a circle of radius aa centred at the origin).

So the Devil’s Curve with a=ba = b consists of the circle x2+y2=a2x^2 + y^2 = a^2 together with the lines y=xy = x and y=−xy = -x.


Part (ii)(a)

With a=2a = 2 and b=5b = \sqrt{5}, the equation is

y2(y2−5)=x2(x2−4).y^2(y^2 - 5) = x^2(x^2 - 4).

Expanding:

y4−5y2=x4−4x2.y^4 - 5y^2 = x^4 - 4x^2.

Rearranging as a quadratic in x2x^2:

(x2)2−4x2−y2(y2−5)=0.(x^2)^2 - 4x^2 - y^2(y^2 - 5) = 0.

For real solutions in xx, the discriminant must be non-negative:

16+4y2(y2−5)⩾0.16 + 4y^2(y^2 - 5) \geqslant 0.

Dividing by 4:

4+y4−5y2⩾0,4 + y^4 - 5y^2 \geqslant 0,

y4−5y2+4⩾0.y^4 - 5y^2 + 4 \geqslant 0.

Factorising:

(y2−1)(y2−4)⩾0.(y^2 - 1)(y^2 - 4) \geqslant 0.

Since y⩾0y \geqslant 0, we can write this as

(y−1)(y+1)(y−2)(y+2)⩾0.(y - 1)(y + 1)(y - 2)(y + 2) \geqslant 0.

As y+1>0y + 1 > 0 and y+2>0y + 2 > 0 for y⩾0y \geqslant 0, the sign is determined by (y−1)(y−2)(y - 1)(y - 2). This product is non-negative when y⩽1y \leqslant 1 or y⩾2y \geqslant 2. Therefore either 0⩽y⩽10 \leqslant y \leqslant 1 or y⩾2y \geqslant 2.


Part (ii)(b)

Very close to the origin: When xx and yy are small, the higher-order terms x4x^4 and y4y^4 are negligible compared to x2x^2 and y2y^2. The equation

y4−5y2=x4−4x2y^4 - 5y^2 = x^4 - 4x^2

becomes approximately

−5y2≈−4x2,-5y^2 \approx -4x^2,

so y2≈45x2y^2 \approx \frac{4}{5}x^2, giving y≈25xy \approx \frac{2}{\sqrt{5}}x (taking the positive root since y⩾0y \geqslant 0). The curve passes through the origin with slope 25\frac{2}{\sqrt{5}}.

Very far from the origin: When xx and yy are large, the x4x^4 and y4y^4 terms dominate. The equation becomes approximately

y4≈x4,y^4 \approx x^4,

so y≈xy \approx x. The curve approaches the line y=xy = x asymptotically.


Part (ii)(c)

Differentiating y4−5y2=x4−4x2y^4 - 5y^2 = x^4 - 4x^2 implicitly with respect to xx:

(4y3−10y)dydx=4x3−8x.(4y^3 - 10y)\frac{dy}{dx} = 4x^3 - 8x.

Tangent parallel to the xx-axis (dydx=0\frac{dy}{dx} = 0):

4x3−8x=0,4x^3 - 8x = 0,

4x(x2−2)=0,4x(x^2 - 2) = 0,

so x=0x = 0 or x=2x = \sqrt{2} (taking x⩾0x \geqslant 0).

  • x=0x = 0: y4−5y2=0y^4 - 5y^2 = 0 gives y2(y2−5)=0y^2(y^2 - 5) = 0, so y=0y = 0 or y=5y = \sqrt{5}.
  • x=2x = \sqrt{2}: y4−5y2=4−8=−4y^4 - 5y^2 = 4 - 8 = -4, so y4−5y2+4=0y^4 - 5y^2 + 4 = 0, giving (y2−1)(y2−4)=0(y^2 - 1)(y^2 - 4) = 0, so y=1y = 1 or y=2y = 2.

At (0,0)(0, 0) the tangent behaviour is degenerate (the curve passes through the origin with a definite slope 25\frac{2}{\sqrt{5}}, but dydx\frac{dy}{dx} takes the indeterminate form 0/00/0). Excluding (0,0)(0, 0), the points with horizontal tangent are:

(0,5),(2,1),(2,2).(0, \sqrt{5}), \quad (\sqrt{2}, 1), \quad (\sqrt{2}, 2).

Tangent parallel to the yy-axis (dxdy=0\frac{dx}{dy} = 0, equivalently 4y3−10y=04y^3 - 10y = 0):

2y(2y2−5)=0,2y(2y^2 - 5) = 0,

so y=0y = 0 or y=52y = \sqrt{\frac{5}{2}}.

  • y=0y = 0: x4−4x2=0x^4 - 4x^2 = 0 gives x2(x2−4)=0x^2(x^2 - 4) = 0, so x=0x = 0 or x=2x = 2.
  • y=52y = \sqrt{\frac{5}{2}}: y2=52y^2 = \frac{5}{2}, so y2(y2−5)=52⋅(−52)=−254y^2(y^2 - 5) = \frac{5}{2} \cdot (-\frac{5}{2}) = -\frac{25}{4}. Then x4−4x2+254=0x^4 - 4x^2 + \frac{25}{4} = 0, with discriminant 16−25=−9<016 - 25 = -9 < 0, so no real xx exists.

Excluding (0,0)(0, 0), the point with vertical tangent is (2,0)(2, 0).

Sketch (first quadrant): The curve has two branches. The first branch starts at the origin (slope 25\frac{2}{\sqrt{5}}), passes through (2,1)(\sqrt{2}, 1) (horizontal tangent), reaches (2,0)(2, 0) (vertical tangent), then continues to (0,5)(0, \sqrt{5}) (horizontal tangent). The second branch starts near the line y=xy = x for large values and comes down to (2,2)(\sqrt{2}, 2) (horizontal tangent), then connects to the asymptotic behaviour.


Part (iii)

The full curve for all x,yx, y is obtained by exploiting the symmetry of the equation. Since the equation involves only x2x^2 and y2y^2 (even powers), the curve is symmetric under x→−xx \to -x and y→−yy \to -y independently. That is, it is symmetric in both the xx-axis and the yy-axis (and hence also under 180∘180^\circ rotation about the origin).

Reflecting the first-quadrant sketch into all four quadrants, the full Devil’s Curve consists of:

  • A closed loop surrounding the origin, passing through (±2,0)(\pm 2, 0) and (0,±5)(0, \pm\sqrt{5}), with four “indentations” at (±2,±1)(\pm\sqrt{2}, \pm 1).
  • A separate component in each quadrant for y⩾2y \geqslant 2, approaching the lines y=±xy = \pm x asymptotically. These four outer branches form a shape resembling a four-pointed star extending to infinity.
Examiner Notes

画图题需标注所有关键点(交点,切线方向变化点);x>=0,y>=0限制下曲线形状与全域不同;y的取值范围分析(0<=y<=1或y>=2)是解题关键。


Topic: 纯数  |  Difficulty: Challenging  |  Marks: 20

8 A pyramid has a horizontal rectangular base ABCDABCD and its vertex VV is vertically above the centre of the base. The acute angle between the face AVBAVB and the base is α\alpha, the acute angle between the face BVCBVC and the base is β\beta and the obtuse angle between the faces AVBAVB and BVCBVC is π−θ\pi - \theta.

(i) The edges ABAB and BCBC are parallel to the unit vectors i and j, respectively, and the unit vector k is vertical. Find a unit vector that is perpendicular to the face AVBAVB.

Show that

cos⁡θ=cos⁡αcos⁡β.\cos \theta = \cos \alpha \cos \beta .

(ii) The edge BVBV makes an angle ϕ\phi with the base. Show that

cot⁡2ϕ=cot⁡2α+cot⁡2β.\cot^2 \phi = \cot^2 \alpha + \cot^2 \beta.

Show also that

cos⁡2ϕ=cos⁡2α+cos⁡2β−2cos⁡2θ1−cos⁡2θ⩾2cos⁡θ−2cos⁡2θ1−cos⁡2θ\cos^2 \phi = \frac{\cos^2 \alpha + \cos^2 \beta - 2 \cos^2 \theta}{1 - \cos^2 \theta} \geqslant \frac{2 \cos \theta - 2 \cos^2 \theta}{1 - \cos^2 \theta}

and deduce that ϕ<θ\phi < \theta.

Hint

(i) If W is centre of base, and M is midpoint of AB, then

MV⃗=λ(0cos⁡αsin⁡α)\vec{MV} = \lambda \begin{pmatrix} 0 \\ \cos \alpha \\ \sin \alpha \end{pmatrix}

M1

So a unit vector perpendicular to AVB is (0−sin⁡αcos⁡α)\begin{pmatrix} 0 \\ -\sin \alpha \\ \cos \alpha \end{pmatrix}

A1 (or B2)

Similarly, a unit vector perpendicular to BVC is (sin⁡β0cos⁡β)\begin{pmatrix} \sin \beta \\ 0 \\ \cos \beta \end{pmatrix}

B1

AS the obtuse angle between AVB and BVC is π−θ\pi - \theta, the acute angle between the two unit vectors is θ\theta, and so

(0−sin⁡αcos⁡α)⋅(sin⁡β0cos⁡β)=cos⁡θ\begin{pmatrix} 0 \\ -\sin \alpha \\ \cos \alpha \end{pmatrix} \cdot \begin{pmatrix} \sin \beta \\ 0 \\ \cos \beta \end{pmatrix} = \cos \theta

M1

Hence cos⁡θ=cos⁡αcos⁡β\cos \theta = \cos \alpha \cos \beta as required.

A1* [5]

(ii) MW=VWcot⁡αMW = VW \cot \alpha, BM=NW=VWcot⁡βBM = NW = VW \cot \beta, BW=VWcot⁡φBW = VW \cot \varphi M1

By Pythagoras, MW2+BM2=BW2MW^2 + BM^2 = BW^2 and so cot⁡2α+cot⁡2β=cot⁡2φ\cot^2 \alpha + \cot^2 \beta = \cot^2 \varphi M1

So

tan⁡2φ=1cot⁡2α+cot⁡2β\tan^2 \varphi = \frac{1}{\cot^2 \alpha + \cot^2 \beta}

and thus

sec⁡2φ=1cot⁡2α+cot⁡2β+1\sec^2 \varphi = \frac{1}{\cot^2 \alpha + \cot^2 \beta} + 1

M1

50


giving

cos⁡2φ=cot⁡2α+cot⁡2βcot⁡2α+cot⁡2β+1=tan⁡2α+tan⁡2βtan⁡2α+tan⁡2β+tan⁡2αtan⁡2β\cos^2 \varphi = \frac{\cot^2 \alpha + \cot^2 \beta}{\cot^2 \alpha + \cot^2 \beta + 1} = \frac{\tan^2 \alpha + \tan^2 \beta}{\tan^2 \alpha + \tan^2 \beta + \tan^2 \alpha \tan^2 \beta}

M1

=sec⁡2α+sec⁡2β−2sec⁡2α+sec⁡2β−2+(sec⁡2α−1)(sec⁡2β−1)= \frac{\sec^2 \alpha + \sec^2 \beta - 2}{\sec^2 \alpha + \sec^2 \beta - 2 + (\sec^2 \alpha - 1)(\sec^2 \beta - 1)}

M1

=cos⁡2α+cos⁡2β−2cos⁡2αcos⁡2βcos⁡2α+cos⁡2β−2cos⁡2αcos⁡2β+(1−cos⁡2α)(1−cos⁡2β)= \frac{\cos^2 \alpha + \cos^2 \beta - 2 \cos^2 \alpha \cos^2 \beta}{\cos^2 \alpha + \cos^2 \beta - 2 \cos^2 \alpha \cos^2 \beta + (1 - \cos^2 \alpha)(1 - \cos^2 \beta)}

M1

=cos⁡2α+cos⁡2β−2cos⁡2θ1−cos⁡2αcos⁡2β= \frac{\cos^2 \alpha + \cos^2 \beta - 2 \cos^2 \theta}{1 - \cos^2 \alpha \cos^2 \beta}

=cos⁡2α+cos⁡2β−2cos⁡2θ1−cos⁡2θ= \frac{\cos^2 \alpha + \cos^2 \beta - 2 \cos^2 \theta}{1 - \cos^2 \theta}

M1 A1* [8]

(cos⁡α−cos⁡β)2≥0(\cos \alpha - \cos \beta)^2 \ge 0

Thus

cos⁡2α+cos⁡2β≥2cos⁡αcos⁡β=2cos⁡θ\cos^2 \alpha + \cos^2 \beta \ge 2 \cos \alpha \cos \beta = 2 \cos \theta

M1

So

cos⁡2φ=cos⁡2α+cos⁡2β−2cos⁡2θ1−cos⁡2θ≥2cos⁡θ−2cos⁡2θ1−cos⁡2θ\cos^2 \varphi = \frac{\cos^2 \alpha + \cos^2 \beta - 2 \cos^2 \theta}{1 - \cos^2 \theta} \ge \frac{2 \cos \theta - 2 \cos^2 \theta}{1 - \cos^2 \theta}

A1* [2]

2cos⁡θ−2cos⁡2θ1−cos⁡2θ=2cos⁡θ(1−cos⁡θ)(1−cos⁡θ)(1+cos⁡θ)\frac{2 \cos \theta - 2 \cos^2 \theta}{1 - \cos^2 \theta} = \frac{2 \cos \theta (1 - \cos \theta)}{(1 - \cos \theta)(1 + \cos \theta)}

1−cos⁡θ≠01 - \cos \theta \neq 0 as θ\theta is acute.

E1

Thus

cos⁡2φ≥2cos⁡θ(1+cos⁡θ)=2(1+cos⁡θ)cos⁡θ\cos^2 \varphi \ge \frac{2 \cos \theta}{(1 + \cos \theta)} = \frac{2}{(1 + \cos \theta)} \cos \theta

As θ\theta is acute, (1+cos⁡θ)<2(1 + \cos \theta) < 2 and so 2(1+cos⁡θ)cos⁡θ>cos⁡θ\frac{2}{(1 + \cos \theta)} \cos \theta > \cos \theta

E1

But also cos⁡θ>cos⁡θcos⁡θ\cos \theta > \cos \theta \cos \theta

E1

Hence, cos⁡2φ≥cos⁡2θ\cos^2 \varphi \ge \cos^2 \theta

51


As both cos⁡φ\cos \varphi and cos⁡θ\cos \theta are positive cos⁡φ≥cos⁡θ\cos \varphi \ge \cos \theta, and so φ≤θ\varphi \le \theta E1 E1 [5]

Model Solution

Part (i)

Set up coordinates with the centre of the base at the origin W=(0,0,0)W = (0, 0, 0). Let the half-lengths of the rectangle be aa along i and bb along j, and let the height of the pyramid be hh. Then:

A=(−a,−b,0),B=(a,−b,0),C=(a,b,0),V=(0,0,h).A = (-a, -b, 0), \quad B = (a, -b, 0), \quad C = (a, b, 0), \quad V = (0, 0, h).

Normal to face AVBAVB: The midpoint of ABAB is M=(0,−b,0)M = (0, -b, 0). The direction from MM to VV is (0,b,h)(0, b, h), which makes angle α\alpha with the base (the horizontal), so tan⁡α=hb\tan\alpha = \frac{h}{b}.

We need a vector perpendicular to face AVBAVB that lies in the plane perpendicular to ABAB. Since ABAB is along i, the normal has no i-component and lies in the yzyz-plane.

Taking the direction from MM to VV as (0,b,h)(0, b, h), a perpendicular direction in the yzyz-plane is (0,−h,b)(0, -h, b). Normalising:

n^1=1b2+h2(0,−h,b).\hat{\mathbf{n}}_1 = \frac{1}{\sqrt{b^2 + h^2}}(0, -h, b).

This normal points inward (toward the interior of the pyramid). We can verify the angle: n^1⋅k=bb2+h2=cos⁡α\hat{\mathbf{n}}_1 \cdot \mathbf{k} = \frac{b}{\sqrt{b^2 + h^2}} = \cos\alpha, confirming α\alpha is the angle between the face and the base.

Normal to face BVCBVC: Similarly, the midpoint of BCBC is N=(a,0,0)N = (a, 0, 0), and the direction from NN to VV is (−a,0,h)(-a, 0, h), making angle β\beta with the base, so tan⁡β=ha\tan\beta = \frac{h}{a}.

A perpendicular to BCBC (which is along j) in the xzxz-plane is (h,0,a)(h, 0, a). Normalising:

n^2=1a2+h2(h,0,a).\hat{\mathbf{n}}_2 = \frac{1}{\sqrt{a^2 + h^2}}(h, 0, a).

Angle between the faces: The obtuse dihedral angle between faces AVBAVB and BVCBVC is π−θ\pi - \theta, so the acute angle between the inward normals is θ\theta. Therefore:

cos⁡θ=n^1⋅n^2=1b2+h2⋅1a2+h2(0⋅h+(−h)(0)+b⋅a)=ab(a2+h2)(b2+h2).\cos\theta = \hat{\mathbf{n}}_1 \cdot \hat{\mathbf{n}}_2 = \frac{1}{\sqrt{b^2 + h^2}} \cdot \frac{1}{\sqrt{a^2 + h^2}}(0 \cdot h + (-h)(0) + b \cdot a) = \frac{ab}{\sqrt{(a^2 + h^2)(b^2 + h^2)}}.

Since cos⁡α=bb2+h2\cos\alpha = \frac{b}{\sqrt{b^2 + h^2}} and cos⁡β=aa2+h2\cos\beta = \frac{a}{\sqrt{a^2 + h^2}}, we have

cos⁡αcos⁡β=bb2+h2⋅aa2+h2=ab(a2+h2)(b2+h2)=cos⁡θ.\cos\alpha \cos\beta = \frac{b}{\sqrt{b^2 + h^2}} \cdot \frac{a}{\sqrt{a^2 + h^2}} = \frac{ab}{\sqrt{(a^2 + h^2)(b^2 + h^2)}} = \cos\theta.

Therefore cos⁡θ=cos⁡αcos⁡β\cos\theta = \cos\alpha \cos\beta.


Part (ii)

Let WW be the centre of the base and MM, NN the midpoints of ABAB, BCBC respectively.

From the right triangle with vertex VV, centre WW, and midpoint MM:

MW=VWcot⁡α.MW = VW \cot\alpha.

Similarly from the right triangle involving NN:

NW=VWcot⁡β.NW = VW \cot\beta.

The edge BVBV makes angle ϕ\phi with the base, so from the right triangle BWVB W V:

BW=VWcot⁡ϕ.BW = VW \cot\phi.

Now B=(a,−b,0)B = (a, -b, 0), M=(0,−b,0)M = (0, -b, 0), N=(a,0,0)N = (a, 0, 0), W=(0,0,0)W = (0, 0, 0).

In the right triangle MBWMBW (right-angled at WW since MWMW is along j and BWBW has components along both i and j… actually let me check):

MW=bMW = b (along j), NW=aNW = a (along i), and BW=a2+b2BW = \sqrt{a^2 + b^2}.

By Pythagoras in triangle MBWMBW:

BW2=MW2+NW2(since MW⊥NW),BW^2 = MW^2 + NW^2 \quad \text{(since $MW \perp NW$)},

so

(VWcot⁡ϕ)2=(VWcot⁡α)2+(VWcot⁡β)2.(VW \cot\phi)^2 = (VW \cot\alpha)^2 + (VW \cot\beta)^2.

Dividing by (VW)2(VW)^2:

cot⁡2ϕ=cot⁡2α+cot⁡2β.\cot^2\phi = \cot^2\alpha + \cot^2\beta.

Deriving cos⁡2ϕ\cos^2\phi: From cot⁡2ϕ=cot⁡2α+cot⁡2β\cot^2\phi = \cot^2\alpha + \cot^2\beta:

tan⁡2ϕ=1cot⁡2α+cot⁡2β,\tan^2\phi = \frac{1}{\cot^2\alpha + \cot^2\beta},

sec⁡2ϕ=1cot⁡2α+cot⁡2β+1=cot⁡2α+cot⁡2β+1cot⁡2α+cot⁡2β.\sec^2\phi = \frac{1}{\cot^2\alpha + \cot^2\beta} + 1 = \frac{\cot^2\alpha + \cot^2\beta + 1}{\cot^2\alpha + \cot^2\beta}.

Therefore:

cos⁡2ϕ=cot⁡2α+cot⁡2βcot⁡2α+cot⁡2β+1=tan⁡2α+tan⁡2βtan⁡2α+tan⁡2β+tan⁡2αtan⁡2β.\cos^2\phi = \frac{\cot^2\alpha + \cot^2\beta}{\cot^2\alpha + \cot^2\beta + 1} = \frac{\tan^2\alpha + \tan^2\beta}{\tan^2\alpha + \tan^2\beta + \tan^2\alpha \tan^2\beta}.

Writing tan⁡2α=sec⁡2α−1\tan^2\alpha = \sec^2\alpha - 1 and tan⁡2β=sec⁡2β−1\tan^2\beta = \sec^2\beta - 1:

Numerator =sec⁡2α+sec⁡2β−2= \sec^2\alpha + \sec^2\beta - 2.

Denominator =(sec⁡2α+sec⁡2β−2)+(sec⁡2α−1)(sec⁡2β−1)= (\sec^2\alpha + \sec^2\beta - 2) + (\sec^2\alpha - 1)(\sec^2\beta - 1)

=sec⁡2α+sec⁡2β−2+sec⁡2αsec⁡2β−sec⁡2α−sec⁡2β+1= \sec^2\alpha + \sec^2\beta - 2 + \sec^2\alpha\sec^2\beta - \sec^2\alpha - \sec^2\beta + 1

=sec⁡2αsec⁡2β−1= \sec^2\alpha\sec^2\beta - 1.

Now multiplying top and bottom by cos⁡2αcos⁡2β\cos^2\alpha\cos^2\beta:

Numerator =sec⁡2α+sec⁡2β−2sec⁡2αsec⁡2β⋅cos⁡2αcos⁡2βcos⁡2αcos⁡2β= \frac{\sec^2\alpha + \sec^2\beta - 2}{\sec^2\alpha\sec^2\beta} \cdot \frac{\cos^2\alpha\cos^2\beta}{\cos^2\alpha\cos^2\beta}

=cos⁡2β+cos⁡2α−2cos⁡2αcos⁡2β= \cos^2\beta + \cos^2\alpha - 2\cos^2\alpha\cos^2\beta.

Denominator =sec⁡2αsec⁡2β−1sec⁡2αsec⁡2β=1−cos⁡2αcos⁡2β= \frac{\sec^2\alpha\sec^2\beta - 1}{\sec^2\alpha\sec^2\beta} = 1 - \cos^2\alpha\cos^2\beta.

Using cos⁡θ=cos⁡αcos⁡β\cos\theta = \cos\alpha\cos\beta from part (i), so cos⁡2αcos⁡2β=cos⁡2θ\cos^2\alpha\cos^2\beta = \cos^2\theta:

cos⁡2ϕ=cos⁡2α+cos⁡2β−2cos⁡2θ1−cos⁡2θ.\cos^2\phi = \frac{\cos^2\alpha + \cos^2\beta - 2\cos^2\theta}{1 - \cos^2\theta}.

The inequality: Since (cos⁡α−cos⁡β)2⩾0(\cos\alpha - \cos\beta)^2 \geqslant 0:

cos⁡2α+cos⁡2β⩾2cos⁡αcos⁡β=2cos⁡θ.\cos^2\alpha + \cos^2\beta \geqslant 2\cos\alpha\cos\beta = 2\cos\theta.

Therefore:

cos⁡2ϕ=cos⁡2α+cos⁡2β−2cos⁡2θ1−cos⁡2θ⩾2cos⁡θ−2cos⁡2θ1−cos⁡2θ.\cos^2\phi = \frac{\cos^2\alpha + \cos^2\beta - 2\cos^2\theta}{1 - \cos^2\theta} \geqslant \frac{2\cos\theta - 2\cos^2\theta}{1 - \cos^2\theta}.

Deducing ϕ<θ\phi < \theta: Factorising the right side:

2cos⁡θ−2cos⁡2θ1−cos⁡2θ=2cos⁡θ(1−cos⁡θ)(1−cos⁡θ)(1+cos⁡θ)=2cos⁡θ1+cos⁡θ,\frac{2\cos\theta - 2\cos^2\theta}{1 - \cos^2\theta} = \frac{2\cos\theta(1 - \cos\theta)}{(1 - \cos\theta)(1 + \cos\theta)} = \frac{2\cos\theta}{1 + \cos\theta},

where we cancelled (1−cos⁡θ)≠0(1 - \cos\theta) \neq 0 since θ\theta is acute.

Now we show 2cos⁡θ1+cos⁡θ>cos⁡2θ\frac{2\cos\theta}{1 + \cos\theta} > \cos^2\theta. Since θ\theta is acute, cos⁡θ>0\cos\theta > 0, so this is equivalent to

21+cos⁡θ>cos⁡θ,\frac{2}{1 + \cos\theta} > \cos\theta,

2>cos⁡θ(1+cos⁡θ)=cos⁡θ+cos⁡2θ.2 > \cos\theta(1 + \cos\theta) = \cos\theta + \cos^2\theta.

2−cos⁡θ−cos⁡2θ>0,2 - \cos\theta - \cos^2\theta > 0,

(1−cos⁡θ)(2+cos⁡θ)>0.(1 - \cos\theta)(2 + \cos\theta) > 0.

Since 0<cos⁡θ<10 < \cos\theta < 1 (as θ\theta is acute), both factors are positive, so this holds.

Therefore cos⁡2ϕ>cos⁡2θ\cos^2\phi > \cos^2\theta. Since both ϕ\phi and θ\theta are acute (so cos⁡ϕ\cos\phi and cos⁡θ\cos\theta are positive), we conclude ϕ<θ\phi < \theta.

Examiner Notes

需正确找到各侧面的法向量;cos(theta)=cos(alpha)cos(beta)是经典立体几何结论;最后的phi<theta不等式证明需巧妙利用已得结果。